Optical fiber amplifier and dispersion compensating fiber module for optical fiber amplifier

ABSTRACT

The invention provides an optical fiber amplifier which assures stable operation of a pump light source and efficiently makes use of residual pump power to achieve improvement in conversion efficiency. The optical fiber amplifier includes a rare earth doped fiber. Pump light from a pump light source is introduced into one end of the rare earth doped fiber by way of a first optical coupler, and residual pump light originating from the pump light and arriving at the other end of the rare earth doped fiber is applied to the other rare earth doped fiber amplifier or the loss compensation of a dispersion compensating fiber by Raman amplification.

CROSS-REFERENCE TO RELATED APPLICATION

This application is a divisional of Ser. No. 11/235,600 filed Sep. 26,2005, which is a continuation of U.S. application Ser. No. 10/834,644filed on Apr. 29, 2004, now U.S. Pat. No. 6,975,447, which is adivisional of U.S. application Ser. No. 09/957,164 filed Sep. 20, 2001,now U.S. Pat. No. 6,747,788, which is a continuation of U.S. applicationSer. No. 08/619,869 filed Mar. 19, 1996, now U.S. Pat. No. 6,342,965 andclaims priority from Japanese Patent Applications 7-061345 filed Mar.20, 1995 and 7-278530 filed Oct. 26, 1995, the contents of which areherein wholly incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates to an optical fiber amplifier and a dispersioncompensating fiber module for use with an optical fiber amplifier.

2. Description of the Related Art

In recent years, research and development of an optical communicationsystem has been and is being performed energetically, and the importanceof booster amplifiers, repeaters or preamplifiers which make use of thetechnique of optical amplification in which an erbium (Er) doped fiber(an erbium-doped-fiber may be hereinafter referred to as “EDF”) isemployed has become apparent.

Further, due to the appearance of optical amplifiers, attention is drawnto an optical-amplifier-repeated transmission system since thetransmission system plays a very important role in achievement ofeconomization of a communication system in the multimedia society.

By the way, in an ordinary rare earth doped fiber optical amplifierwhich particularly amplifies a wavelength of a signal, the length of thedoped fiber is set to a value at which a maximum gain is obtained inorder to assure a high conversion efficiency from pump power to signalpower.

Meanwhile, in a wavelength division multiplexing (WDM) optical amplifierwhich amplifies many channels at the same time, it is important to keepthe wavelength dependency of the gain as flat as possible. As a result,the rare earth doped fiber (which will be hereinafter discussed inconnection with a representative EDF) must operate in a conditionwherein the degree of the saturation of the gain is low. To this end,where the concentration of high level ions is represented by N2 whilethe concentration of all ions is represented by N1 and N2/N1 is definedas pump ratio, in order to raise the average pump ratio N2/N1 of thedoped fiber over the entire length, the length of the doped fiber mustbe set short.

However, if the doped fiber is formed short in this manner, then muchresidual pump power will leak out from the other end of the doped fiber,resulting in degradation of the conversion efficiency. Nevertheless,since the required pump power increases as the number of signalwavelengths increases, the output power of a semiconductor pump lasermust be raised.

In particular, although it is apparent from the conservative law ofenergy that the pump power increases as the number of wavelengthsincreases, a wavelength multiplexing optical amplifier cannot be used ina condition in which it exhibits a high efficiency of conversion frompump power to signal power. This is because, since the rare earth dopedfiber is intentionally formed short so as to prevent saturation in orderto obtain a gain over a wide bandwidth or to make the gain flat, pumppower which has not been converted into a signal will leak out from theother end of the doped fiber.

Accordingly, while high pump power is required originally when comparingwith ordinary amplification of only one signal channel, the rare earthdoped fiber must be used in a condition wherein the pump power leaks outtherefrom.

Thus, in order to effectively make use of thus leaking out residual pumplight, a technique has been proposed wherein a reflecting mirror isprovided at the other end of a doped fiber so that residual pump lightis reflected by the reflecting mirror so as to be introduced back intothe doped fiber so that it may be used for optical amplification again.The technique is disclosed in Japanese Patent Laid-Open Application No.Heisei 3-25985 or Japanese Patent Laid-Open Application No. 3-166782.

However, where residual pump light is reflected by the reflecting mirrorin this manner, the pump light is returned not only to the doped fiberbut also to the pump source. This pump light may possibly give rise tounstable operation of the pump source such as interference.

By the way, while, due to the appearance of optical amplifiers,attention is drawn to an optical-amplifier-repeated transmission systemwhich includes a plurality of repeating and amplifying opticalamplifiers since it plays a very important role in achievement ofeconomization of a communication system in the multimedia society asdescribed above, the transmission system has subjects to be solved interms of the dispersion compensation, reduction in nonlinear effects(effects having a bad influence on the transmission quality) in anoptical fiber serving as a transmission line and economic wide bandwidthwavelength multiplexing transmission.

Generally, an optical fiber serving as a transmission line has adispersion characteristic and accumulates a dispersion amount inproportion to the length thereof. Usually, however, in an optical fibertransmission system which employs regenerative repeaters, the dispersionamount is reset at the regenerative repeaters. Consequently, theaccumulation of the dispersion amount does not make a problem.

However, in an optical-amplifier-repeated transmission system, since atransmitted optical signal is repeated by a kind of analogamplification, the dispersion amount is accumulated. Accordingly, inorder to eliminate the accumulation, the signal wavelength used fortransmission should be set to a zero dispersion wavelength. This,however, provides the following subjects to be solved:

1-1) Optical fibers have already been laid by a large amount, andunfortunately, those optical fibers have a zero dispersion wavelength at1.3 μm while an optical amplifier which is expected to be put intopractical use soon can amplify only a signal of the 1.55 μm band;

1-2) It has been reported recently that, even if optical fibers whosezero dispersion wavelength is 1.55 μm are laid newly to transmit asignal of 1.55 μm, nonlinear effects occur actively in the opticalfibers. This signifies that, if a signal wavelength equal to a zerodispersion wavelength is used for transmission, then undesirablenonlinear effects occur; and

1-3) Particularly in wavelength multiplexing transmission, since aplurality of different signal wavelengths are involved, the concept thatthe signal wavelengths are set equal to a zero dispersion wavelengthcannot be applied.

Accordingly, it has been proposed recently to intentionally displace thesignal wavelength from the zero dispersion wavelength suitably andcompensate for the dispersion, for example, at the repeater.

While research of dispersion compensators has been and is beingperformed actively in recent years in this manner, one of dispersioncompensators which is expected to be most likely put into practical useis a dispersion compensating fiber (which may be referred to as “DCF”;here the term DCF is the abbreviation of Dispersion Compensating Fiber).The DCF, however, has the following subjects to be solved:

2-1) Where fibers (transmission lines) laid already are utilized, adispersion compensating fiber must be interposed as a device at eachrepeating point in order to perform dispersion compensation collectivelyat such each repeating point. Therefore, research and development isbeing directed to reduction in length of dispersion compensating fibers.

2-2) When fibers are to be laid newly, it is a possible idea not tointerpose a dispersion compensating fiber as a device but to lay adispersion compensating fiber as part of a transmission line. Forexample, a transmission line of 40 km may be formed from a fiber of 20km and a dispersion compensating fiber of 20 km. However, research anddevelopment of such a novel dispersion compensating fiber as justmentioned makes overlapping development with research and development ofa dispersion compensating fiber for the application described inparagraph 2-1) above.

In summary, in wavelength multiplexing transmission, a wavelengthdispersion must be compensated for, and since the compensation for awavelength dispersion is expected to be most likely put into practicaluse where a dispersion compensating fiber is employed, it is prospectiveto use a dispersion compensating fiber. Further, it is investigated toincorporate a dispersion compensating fiber as a part into an opticalamplifier repeater. Generally, however, the mode field diameter of adispersion compensating fiber (DCF) is set small in order to compensatefor a dispersion, and consequently, nonlinear effects are liable tooccur and, as the dispersion amount to be compensated for increases,also the loss increases.

Thus, it is a possible method to compensate also for the loss of adispersion compensating fiber using an optical amplifier. In thisinstance, the loss must be compensated for so that a transmissionoptical signal may not be influenced by nonlinear effects which degradethe quality of a signal such as self-phase modulation (SPM) andcross-phase modulation (XPM) occurring in the dispersion compensatingfiber. Accordingly, the possible method has a problem in that designingof a level diagram is difficult. Further, while a flat and wide opticalamplification bandwidth is required for an optical amplifier for WDM,also a rare earth doped fiber optical amplifier has a wavelengthdependency of the gain. Accordingly, there is a subject to be solved inthat it is difficult to realize a flat and wide amplification bandwidth.

Meanwhile, a rare earth doped fiber optical amplifier having a high gainsometimes suffers from unnecessary oscillations which are produced whenit performs optical amplification. If such unnecessary oscillations areproduced, the rare earth doped fiber optical amplifier operates butunstably.

For example, in an erbium-doped-fiber optical amplifier, spontaneousemission light (ASE) of 1.53 to 1.57 μm in wavelength is generated whenoptical amplification is performed, and since the ASE is repetitivelyreflected from reflection points in the erbium-doped-fiber opticalamplifier, unnecessary oscillations are liable to be produced.Particularly with an erbium-doped-fiber optical amplifier adjusted formultiple wavelength collection amplification (that is, anerbium-doped-fiber optical amplifier having a high pump rate), since ithas a high gain in the proximity of 1.53 μm, unnecessary oscillationsare liable to be produced at this wavelength. When such unnecessaryoscillations are produced, the erbium-doped-fiber optical amplifieroperates but unstably.

SUMMARY OF THE INVENTION

It is an object of the present invention to provide an optical fiberamplifier wherein stable operation of a pump source (pump light source)is assured and residual pump power which is produced when the averagepump ratio is raised is utilized efficiently to improve the conversionefficiency.

It is another object of the present invention to provide an opticalfiber amplifier and a dispersion compensating fiber module for anoptical fiber amplifier employing a dispersion compensating fiberwherein the loss of the dispersion compensating fiber by Ramanamplification can be compensated for making use of the fact that thethreshold value of the Raman amplification is low because the mode fielddiameter of the dispersion compensating fiber is small.

It is a further object of the present invention to provide an opticalfiber amplifier wherein, where a silica-type-optical-fiber having aRaman amplification function similarly to a dispersion compensatingfiber is employed, the loss Of the silica-type-optical-fiber by Ramanamplification can be compensated for similarly to the case where adispersion compensating fiber is used.

It is a still further object of the present invention to provide anoptical fiber amplifier which minimizes unstable operation of a rareearth doped fiber optical amplifier having a high gain or a rare earthdoped fiber optical amplifier adjusted for multiple wavelengthcollective amplification.

In order to attain the objects of the present invention described above,according to an aspect of the present invention, there is provided anoptical fiber amplifier including a rare earth doped fiber, whichcomprises first means for introducing pump light into one end of therare earth doped fiber by way of a first optical coupler, second meansfor demultiplexing residual pump light originating from the pump lightintroduced into the one end of the rare earth doped fiber by the firstmeans and arriving at the other end of the rare earth doped fiber by asecond optical coupler and reflecting the demultiplexed residual pumplight by reflection means so as to be introduced back into the rareearth doped fiber, and third means for preventing the residual pumplight introduced back into the rare earth doped fiber by the secondmeans from being introduced into a pump source, from which the pumplight to be introduced into the rare earth doped fiber by the firstmeans is produced, by optical isolation means so as to prevent unstableoperation of the pump source.

In the optical fiber amplifier, when pump light is introduced into theone end of the rare earth doped fiber by way of the first opticalcoupler, residual pump light arrives at the other end of the rare earthdoped fiber and is then demultiplexed by the second optical coupler,whereafter it is reflected by the reflection means so that it isintroduced back into the rare earth doped fiber. In order to preventunstable operation of the pump source caused by interference of theresidual pump light introduced back into the rare earth doped fiber, theoptical isolation means is interposed between the pump source and thefirst optical coupler. Consequently, the optical fiber amplifier isadvantageous in that it makes use of the pump power with a highefficiency while assuring stabilized operation of the pump source.

According to another aspect of the present invention, there is providean optical fiber amplifier including a rare earth doped fiber, whichcomprises a pump source, a first optical coupler for introducing pumplight from the pump source into one end of the rare earth doped fiber, asecond optical coupler for demultiplexing residual pump lightoriginating from the pump light introduced into the one end of the rareearth doped fiber by way of the first optical coupler and arriving atthe other end of the rare earth doped fiber, a reflecting mirror forreflecting the residual pump light demultiplexed by the second opticalcoupler so as to be introduced back into the rare earth doped fiber byway of the second optical coupler, and an optical isolator interposedbetween the pump source and the first optical coupler for preventingunstable operation of the pump source arising from interference of theresidual pump light introduced back into the rare earth doped fiber.

In the optical fiber amplifier, when pump light is introduced into theone end of the rare earth doped fiber by way of the first opticalcoupler, residual pump light arrives at the other end of the rare earthdoped fiber and is demultiplexed by the second optical coupler,whereafter it is reflected by the reflecting mirror so that it isintroduced back into the rare earth doped fiber. In order to preventunstable operation of the pump source caused by interference of theresidual pump light introduced back into the rare earth doped fiber, theoptical isolator is interposed between the pump source and the firstoptical coupler. Consequently, the optical fiber amplifier isadvantageous in that it makes use of the pump power with a highefficiency while assuring stabilized operation of the pump source.

According to a further aspect of the present invention, there isprovided an optical fiber amplifier including a first rare earth dopedfiber and a second rare earth doped fiber disposed at front and rearstages, which comprises first means for introducing pump light into oneend of one of the first rare earth doped fiber and the second rare earthdoped fiber by way of an optical circulator having three or more portsand a first optical coupler, second means for demultiplexing residualpump light originating from the pump light introduced into the one endof the one rare earth doped fiber by the first means and arriving at theother end of the one rare earth doped fiber by a second optical couplerand reflecting the demultiplexed residual pump light by reflection meansso as to be introduced back into the one rare earth doped fiber, andthird means for causing the residual pump light reflected from thereflection means and introduced back into the one rare earth doped fiberby the second means to follow, after passing the one rare earth dopedfiber, a different optical path by the optical circulator andmultiplexing the residual pump light in the different optical path withan output of the other one of the first rare earth doped fiber and thesecond rare earth doped fiber by a third optical coupler.

In the optical fiber amplifier, pump light is first passed through theoptical circulator having three or more ports and then introduced intothe one end of the rare earth doped fiber at the front stage or the rearstage by the first optical coupler. Then, residual pump lightoriginating from the pump light and arriving at the other end of therare earth doped fiber is demultiplexed by the second optical couplerand then reflected by the reflection means so that it is introduced backinto the rare earth doped fiber. The residual pump light is thenintroduced, after passing the rare earth doped fiber, into the differentoptical path by the optical circulator and is multiplexed with an outputof the other rare earth doped fiber by the third optical coupler.Consequently, the optical fiber amplifier of the two stage constructionjust described is advantageous in that it makes use of the pump powerwith a high efficiency.

According to a still further aspect of the present invention, there isprovided an optical fiber amplifier including a first rare earth dopedfiber and a second rare earth doped fiber disposed at front and rearstages, which comprises a pump source, a first optical coupler providedat one end of one of the first rare earth doped fiber and the secondrare earth doped fiber, a second optical coupler provided at the otherend of the one rare earth doped fiber, a third optical coupler providedat one end of the other one of the first rare earth doped fiber and thesecond rare earth doped fiber, a reflecting mirror for reflectingresidual pump light demultiplexed by the second optical coupler so as tobe introduced back into the one rare earth doped fiber by way of thesecond optical coupler, and an optical circulator having three or moreports connected to the pump source, the first optical coupler and thethird optical coupler, and wherein pump light from the pump source isintroduced into one end of the one rare earth doped fiber by way of theoptical circulator and the first optical coupler, and residual pumplight originating from the pump light introduced into the one end of theone rare earth doped fiber and arriving at the other end of the one rareearth doped fiber is demultiplexed by the second optical coupler andreflected by the reflecting mirror so as to be introduced back into theone rare earth doped fiber, whereafter the residual pump light isintroduced, after passing the one rare earth doped fiber, into adifferent optical path by the optical circulator so that the residualpump light is thereafter multiplexed with an output of the other rareearth doped fiber by the third optical coupler.

The optical fiber amplifier of the two stage construction just describedis advantageous in that it makes use of the pump power with a highefficiency.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier including a first rare earth dopedfiber and a second rare earth doped fiber disposed at front and rearstages, which comprises first means for branching pump power at a ratioof n:1, n being a real number equal to or greater than 1, by an opticalbranching element, multiplexing the pump light from a port of theoptical branching element by a first optical coupler and introducing themultiplexed light into one end of one of the first rare earth dopedfiber and the second rare earth doped fiber, second means for extractingresidual pump power originating from the pump light introduced Into theone end of the one rare earth doped fiber by the first means andarriving at the other end of the one rare earth doped fiber by a secondoptical coupler connected to the other end of the one rare earth dopedfiber, multiplexing the extracted residual pump power by a third opticalcoupler and introducing the multiplexed power into one end of the otherone of the first rare earth doped fiber and the second rare earth dopedfiber, and third means for multiplexing the pump power from another portof the optical branching element branched by the optical branchingelement and introducing the multiplexed power into the other end of theother rare earth doped fiber by a fourth optical coupler.

In the optical fiber amplifier, the pump power is branched at the ratioof n:1, and the pump light from a port of the optical branching elementis multiplexed by the first optical coupler and then introduced into therare earth doped fiber at the front stage or the rear stage. Then,residual pump power is extracted by the second optical coupler connectedto the other end of the rare earth doped fiber and is then multiplexedby the third optical coupler. Then, the output light of the thirdoptical coupler is introduced into the one end of the other rare earthdoped fiber. Meanwhile, the branched pump power from another port of theoptical branching element is introduced into the other end of andmultiplexed in the other rare earth doped fiber by the fourth opticalcoupler. Consequently, the optical fiber amplifier of the two stageconstruction just described is advantageous in that it makes use of thepump power with a high efficiency.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier including a first rare earth dopedfiber and a second rare earth doped fiber disposed at front and rearstages, which comprises a pump source, an optical branching element forbranching pump power from the pump source at a ratio of n:1, n being areal number equal to or greater than 1, a first optical coupler formultiplexing the pump light from a port of the optical branching elementand introducing the multiplexed light into one of the first rare earthdoped fiber and second rare earth doped fiber, a second optical couplerfor extracting residual pump power outputted from the one rare earthdoped fiber, a third optical coupler for multiplexing the residual pumppower extracted by the second optical coupler and introducing themultiplexed power into the other one of the first rare earth doped fiberand the second rare earth doped fiber, and a fourth optical coupler formultiplexing the pump power from another port of the optical branchingelement branched by the optical branching element and introducing themultiplexed power into the other rare earth doped fiber.

In the optical fiber amplifier, the pump power is branched at the ratioof n:1, and the pump light from a port of the optical branching elementis multiplexed by the first optical coupler and then introduced into therare earth doped fiber at the front stage or the rear stage. Then,residual pump power is extracted by the second optical coupler connectedto the other end of the rare earth doped fiber and is then multiplexedby the third optical coupler. Then, the output light of the thirdoptical coupler is introduced into the one end of the other rare earthdoped fiber. Meanwhile, the branched pump power from another port of theoptical branching element is introduced into the other end of andmultiplexed in the other rare earth doped fiber by the fourth opticalcoupler. Consequently, the optical fiber amplifier of the two stageconstruction just described is advantageous in that it makes use of thepump power with a high efficiency.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier including a rare earth doped fiber,which comprises a pump source, an optical circulator having three ormore ports one of which is connected to the pump source, a first opticalcoupler for multiplexing pump light introduced thereto from the pumpsource by way of the optical circulator and introducing the multiplexedlight into one end of the rare earth doped fiber, a second opticalcoupler for demultiplexing residual pump light originating from the pumplight introduced into the one end of the rare earth doped fiber by thefirst optical coupler and arriving at the other end of the rare earthdoped fiber, a reflecting mirror for reflecting the residual pump lightdemultiplexed by the second optical coupler so as to be introduced backinto the rare earth doped fiber by way of the second optical coupler, aresidual pump light detector for detecting the residual pump lightintroduced back into the rare earth doped fiber by the reflecting mirrorand inputted from the one end of the rare earth doped fiber to theoptical circulator by way of the first optical coupler, and a controllerfor controlling the pump source so that the residual pump light detectedby the residual pump light detector may be constant.

In the optical fiber amplifier, pump light is first passed through theoptical circulator having three or more ports and is then introducedinto the one end of the rare earth doped fiber by the first opticalcoupler. Then, residual pump light originating from the pump light andarriving at the other end of the rare earth doped fiber is demultiplexedby the second optical coupler and then reflected by the reflectingmirror so that it is introduced back into the rare earth doped fiber.The residual pump power comes out from the one end of the rare earthdoped fiber and is then inputted by way of the first optical coupler tothe optical circulator, by which it is introduced into the differentoptical path so that it is monitored by the residual pump lightdetector. Then, the residual pump power is kept constant under thecontrol of the controller. Consequently, the wavelength characteristicof the gain of the optical fiber amplifier can be controlled so that itmay not be varied irrespective of any variation of the input level.Consequently, the optical fiber amplifier is advantageous in that it canbe realized readily as a multiple wavelength collective amplifier.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth dopedfiber, and a Raman optical amplification element which is pumped withpump light to cause Raman amplification to occur, the rare earth dopedfiber optical amplification element and the Raman optical amplificationelement being connected in cascade connection.

The optical fiber amplifier is advantageous in that it makes use of thepump power with a high efficiency while it has a two stage construction.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth dopedfiber, a Raman optical amplification element which is pumped with pumplight, which is capable of pumping the rare earth doped fiber opticalamplification element, to cause Raman amplification to occur, the rareearth doped fiber optical amplification element and the Raman opticalamplification element being connected in cascade connection, and a pumpsource for supplying pump light for pumping the rare earth doped fiberoptical amplification element and the Raman optical amplificationelement.

In the optical fiber amplifier, since it includes the pump source forsupplying pump light for pumping the rare earth doped fiber opticalamplification element and the Raman optical amplification element, thepump power can be utilized with a high efficiency and the number of pumpsources to be used can be reduced, which contributes to simplificationin construction and reduction in cost.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth dopedfiber, and a Raman optical amplification element formed from adispersion compensating fiber which is pumped with pump light to causeRaman amplification to occur, the rare earth doped fiber opticalamplification element and the Raman optical amplification element beingconnected in cascade connection at two front and rear stages.

The optical fiber amplifier just described is advantageous in that itmakes use of the pump power with a high efficiency while it has a twostage construction.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber and a dispersion compensating fiber disposed at two front and rearstages, a first pump source for producing pump light of a firstwavelength band for the rare earth doped fiber, a first optical couplerfor introducing the pump light from the first pump source into the rareearth doped fiber, a second pump source for producing pump light of asecond wavelength band for the dispersion compensating fiber, and asecond optical coupler for introducing the pump light from the secondpump source into the dispersion compensating fiber, the dispersioncompensating fiber being pumped with the pump light of the secondwavelength band from the second pump source to cause Raman amplificationto occur.

With the optical fiber amplifier, compensation for the loss of thedispersion compensating fiber by Raman amplification can be achievedwhile optical amplification is performed by the rare earth doped fiber.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises anerbium-doped-fiber and a dispersion compensating fiber disposed at twofront and rear stages, a pump source for producing pump light, and anoptical coupler for introducing the pump light from the pump source intothe erbium-doped-fiber, the dispersion compensating fiber being pumpedwith residual pump light from the erbium-doped-fiber to cause Ramanamplification to occur.

With the optical fiber amplifier, compensation for the loss of thedispersion compensating fiber by Raman amplification can be achievedwhile optical amplification is performed by the erbium-doped-fiber.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises anerbium-doped-fiber and a dispersion compensating fiber disposed at twofront and rear stages, a pump source for producing pump light, and anoptical coupler for introducing the pump light from the pump source intothe dispersion compensating fiber, the erbium-doped-fiber being pumpedwith residual pump light from the dispersion compensating fiber.

With the optical fiber amplifier, compensation for the loss of thedispersion compensating fiber by Raman amplification can be achievedwhile optical amplification is performed by the erbium-doped-fiber.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a dispersioncompensating fiber doped with a rare earth element, a pump source forproducing pump light for the dispersion compensating fiber, and anoptical coupler for introducing the pump light from the pump source intothe dispersion compensating fiber.

With the optical fiber amplifier, since the dispersion compensatingfiber used is doped with a rare earth element, dispersion compensationcan be performed by the dispersion compensating fiber, and the loss ofthe dispersion compensating fiber can be reduced simultaneously. Theoptical fiber amplifier with the dispersion compensation function isadvantageous also in that it can optically amplify signal lightsufficiently.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises anerbium-doped-fiber and a dispersion compensating fiber disposed at twofront and rear stages, a pump source for producing pump light for theerbium-doped-fiber, an optical coupler for introducing the pump lightfrom the pump source into the erbium-doped-fiber, and an optical filterinterposed between the erbium-doped-fiber and the dispersioncompensating fiber for intercepting residual pump light coming out fromthe erbium-doped-fiber.

With the optical fiber amplifier, leakage pump power Raman amplifies thedispersion compensating fiber. Consequently, the optical fiber amplifieris prevented from unstable operation or from variation of the wavelengthdependency of the amplification band thereof.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth dopedfiber, and a Raman optical amplification element formed from asilica-type-optical-fiber which causes, when pumped with pump light,Raman amplification to occur, the rare earth doped fiber opticalamplification element and the Raman optical amplification element beingconnected in cascade connection at two front and rear stages.

The optical fiber amplifier just described is advantageous in that itmakes use of the pump power with a high efficiency while it has a twostage construction.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises asilica-type-optical-fiber and an erbium-doped-fiber provided at a frontstage and a rear stage, respectively, a silica-type-optical-fiber pumpsource for producing pump light of a wavelength band for thesilica-type-optical-fiber, an optical coupler for introducing the pumplight from the silica-type-optical-fiber pump source into thesilica-type-optical-fiber, an erbium-doped-fiber pump source forproducing pump light of a wavelength band for the erbium-doped-fiber,and another optical coupler for introducing the pump light from theerbium-doped-fiber pump source into the erbium-doped-fiber, thesilica-type-optical-fiber being pumped with the pump light from thesilica-type-optical-fiber pump source to cause Raman amplification tooccur.

With the optical fiber amplifier, compensation for the loss of thesilica-type-optical-fiber by Raman amplification can be performed whileoptical amplification by the erbium-doped-fiber is performed.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises anerbium-doped-fiber having a low noise figure and asilica-type-optical-fiber provided at a front stage and a rear stage,respectively, a silica-type-optical-fiber pump source for producing pumplight of a wavelength band for the silica-type-optical-fiber, an opticalcoupler for introducing the pump light from thesilica-type-optical-fiber pump source into thesilica-type-optical-fiber, an erbium-doped-fiber pump source forproducing pump light of a wavelength band for the erbium-doped-fiber,and another optical coupler for introducing the pump light from theerbium-doped-fiber pump source into the erbium-doped-fiber, thesilica-type-optical-fiber being pumped with the pump light from thesilica-type-optical-fiber pump source to cause Raman amplification tooccur.

With the optical fiber amplifier, compensation for the loss of thesilica-type-optical-fiber by Raman amplification can be performed whileoptical amplification by the erbium-doped-fiber is performed.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth doped fiberand having a low noise figure, the rare earth doped fiber opticalamplification element being disposed as a front stage amplificationelement, a Raman optical amplification element for causing Ramanamplification to occur when pumped with pump light, the Raman opticalamplification section being disposed as a middle stage amplificationelement, and another rare earth doped fiber optical amplificationelement formed from a rare earth doped fiber and disposed as a rearstage amplification element.

With the optical fiber amplifier, the compensation effect of the Ramanoptical amplification element can be increased. Consequently, a widebandwidth optical amplifier can be realized while achievingsimplification in structure and reduction in cost.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a firsterbium-doped-fiber having a low noise figure, a dispersion compensatingfiber and a second erbium-doped-fiber provided at a front stage, amiddle stage and a rear stage, respectively, a first erbium-doped-fiberpump source for producing pump light of a wavelength band for the firsterbium-doped-fiber, an optical coupler for introducing the pump lightfrom the first erbium-doped-fiber pump source into the firsterbium-doped-fiber, a dispersion compensating fiber pump source forproducing pump light of a wavelength band for the dispersioncompensating fiber, another optical coupler for introducing the pumplight from the dispersion compensating fiber pump source into thedispersion compensating fiber, a second erbium-doped-fiber pump sourcefor producing pump light of a wavelength band for the seconderbium-doped-fiber, and a further optical coupler for introducing thepump light from the second erbium-doped-fiber pump source into thesecond erbium-doped-fiber, the dispersion compensating fiber beingpumped with the pump light from the dispersion compensating fiber pumpsource to cause Raman amplification to occur.

With the optical fiber amplifier, the compensation effect of the Ramanoptical amplification element can be increased. Consequently, a widebandwidth optical amplifier can be realized while achievingsimplification in structure and reduction in cost.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a firsterbium-doped-fiber having a low noise figure, asilica-type-optical-fiber and a second erbium-doped-fiber provided at afront stage, a middle stage and a rear stage, respectively, a firsterbium-doped-fiber pump source for producing pump light of a wavelengthband for the first erbium-doped-fiber, an optical coupler forintroducing the pump light from the first erbium-doped-fiber pump sourceinto the first erbium-doped-fiber, a silica-type-optical-fiber pumpsource for producing pump light of a wavelength band for thesilica-type-optical-fiber, another optical coupler for introducing thepump light from the silica-type-optical-fiber pump source into thesilica-type-optical-fiber, a second erbium-doped-fiber pump source forproducing pump light of a wavelength band for the seconderbium-doped-fiber, and a further optical coupler for introducing thepump light from the second erbium-doped-fiber pump source into thesecond erbium-doped-fiber, the silica-type-optical-fiber being pumpedwith the pump light from the silica-type-optical-fiber pump source tocause Raman amplification to occur.

With the optical fiber amplifier, the compensation effect of thesilica-type-optical-fiber can be increased. Consequently, a widebandwidth optical amplifier can be realized while achievingsimplification in structure and reduction in cost.

According to a yet further aspect of the present invention, there isprovided a dispersion compensating fiber module for an optical fiberamplifier, which comprises a dispersion compensating fiber, and a pumpsource for pumping the dispersion compensating fiber to cause Ramanamplification to occur.

Where an optical fiber amplifier is constructed using the module whereinthe dispersion compensating fiber is pumped to cause Raman amplificationto occur, it exhibits a reduced loss due to reduction of the loss by thedispersion compensating fiber.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier including a dispersion compensatingfiber, which comprises a pump source, and an optical coupler forintroducing pump light from the pump source into the dispersioncompensating fiber, the dispersion compensating fiber being pumped withpump light from the pump source to cause Raman amplification to occur.

Also the optical fiber amplifier is advantageous in that the loss of thedispersion compensating fiber can be reduced.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a pump source, andan optical coupler for introducing pump light from the pump source intothe silica-type-optical-fiber, the silica-type-optical-fiber beingpumped with the pump light from the pump source to cause Ramanamplification to occur.

The optical fiber amplifier is advantageous in that the loss of thesilica-type-optical-fiber can be reduced.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises a rare earth dopedfiber optical amplification element formed from a rare earth dopedfiber, and an optical fiber attenuation element formed from an opticalfiber or an optical fiber with an optical isolator for suppressingunstable operation of the rare earth doped fiber optical amplificationelement.

The optical fiber amplifier is advantageous in that stabilized opticalamplification can be achieved with unstable operation of the rare earthdoped fiber optical amplification element suppressed.

According to a yet further aspect of the present invention, there isprovided an optical fiber amplifier, which comprises an opticalamplification unit including a front stage optical amplification elementand a rear stage optical amplification element each formed as a rareearth doped fiber optical amplification element formed from a rare earthdoped fiber, and an optical fiber attenuation element formed from anoptical fiber or an optical fiber with an optical isolator interposedbetween the front stage optical amplification element and the rear stageoptical amplification element of the optical amplification unit forsuppressing unstable operation of the optical amplification unit.

The optical fiber amplifier is advantageous in that stabilized opticalamplification can be achieved with unstable operation of the opticalamplification unit suppressed.

Further objects, features and advantages of the present invention willbecome apparent from the following detailed description when read inconjunction with the accompanying drawings in which like parts orelements are denoted by like reference characters.

BRIEF DESCRIPTION OF THE DRAWING

FIGS. 1 to 9, 10(a), 10(b), 11, 12, 13(a), 13(b), 14 and 15 are blockdiagrams illustrating different aspects of the present invention;

FIG. 16 is a block diagram of an optical fiber amplifier showing a firstpreferred embodiment of the present invention;

FIGS. 17 to 20 are block diagrams showing different modifications to theoptical amplifier of FIG. 16;

FIG. 21 is an electric circuit diagram showing a constant optical outputcontrol system shown in FIG. 20;

FIG. 22 is a table illustrating operation of the constant optical outputcontrol system of FIG. 21;

FIG. 23 is a block diagram of another optic&l fiber amplifier showing asecond preferred embodiment of the present invention;

FIG. 24 is a block diagram showing a modification to the optical fiberamplifier of FIG. 23;

FIGS. 25 to 27 are block diagrams of further optical fiber amplifiersshowing third, fourth and fifth preferred embodiment of the presentinvention, respectively;

FIG. 28 is an electric circuit diagram showing a constant pump lightoutput control system shown in FIG. 27;

FIG. 29 is a table illustrating operation of the constant pump lightoutput control system of FIG. 28;

FIGS. 30 and 31 are block diagrams showing different modifications tothe optical fiber amplifier of FIG. 27;

FIG. 32 is a block diagram of a still further optical fiber amplifiershowing a sixth preferred embodiment of the present invention;

FIG. 33 is a block diagram showing a modification to the optical fiberamplifier of FIG. 32;

FIGS. 34 and 35 are block diagrams of yet further optical fiberamplifiers showing seventh and eighth preferred embodiments of thepresent invention, respectively;

FIGS. 36 and 37 are block diagrams showing different modifications tothe optical fiber amplifier of FIG. 35;

FIGS. 38 to 43 are block diagrams of yet further optical fiberamplifiers showing ninth, tenth, eleventh, twelfth, thirteenth andfourteenth preferred embodiments of the present invention, respectively;

FIGS. 44 and 45 are block diagrams showing different modifications tothe optical fiber amplifier of FIG. 43;

FIGS. 46 and 47 are diagrams illustrating wavelength characteristics ofan optical fiber amplifier;

FIG. 48 is a block diagram of a yet further optical fiber amplifiershowing a fifteenth preferred embodiment of the present invention;

FIG. 49 is a block diagram showing a modification to the optical fiberamplifier of FIG. 48;.

FIG. 50 is a block diagram of a yet further optical fiber amplifiershowing a sixteenth preferred embodiment of the present invention;

FIGS. 51 and 52 are block diagrams showing different modifications tothe optical fiber amplifier of FIG. 50;

FIGS. 53( a) and 53(b) are schematic views showing a construction of anoptical circulator;

FIGS. 54( a) and 54(b) are schematic views showing a construction of anisolator.

FIG. 55 is a block diagram of a yet further optical fiber amplifiershowing a seventeenth preferred embodiment of the present invention; and

FIGS. 56 to 58 are block diagrams showing different modifications to theoptical fiber amplifier of FIG. 55.

DESCRIPTION OF THE PREFERRED EMBODIMENTS A. Aspects of the Invention

Several aspects of the present invention will first be described withreference to FIGS. 1 to 9, 10(a), 10(b), 11, 12, 13(a), 13(b), 14 and15.

A1. First Aspect of the Invention

Referring first to FIG. 1, there is shown in block diagram an opticalfiber amplifier according to a first aspect of the present invention.The optical fiber amplifier shown includes a rare earth doped fiber 1,and a pump source (pump light source) 2. The optical fiber amplifierfurther includes a first optical coupler 3-1 for introducing pump lightfrom the pump source 2 Into one end of the rare earth doped fiber 1, anda second optical coupler 3-2 for demultiplexing residual pump lightoriginating from the pump light introduced into the one end of the rareearth doped fiber 1 by way of the first optical coupler 3-1 and arrivingat the other end of the rare earth doped fiber 1.

The optical fiber amplifier further includes a reflecting mirror 4 forreflecting residual pump light demultiplexed by the second opticalcoupler 3-2 so as to be introduced back into the rare earth doped fiber1 by way of the second optical coupler 3-2. The optical fiber amplifierfurther includes an optical isolator 5 interposed between the pumpsource 2 and the first optical coupler 3-1 for preventing unstableoperation of the pump source 2 arising from interference of the residualpump light introduced back into the rare earth doped fiber 1.

In this instance, the optical fiber amplifier shown in FIG. 1 andincluding the rare earth doped fiber 1 is constructed such that itincludes a first system for introducing pump light into one end of therare earth doped fiber 1 by way of a first optical coupler 3-1, a secondsystem for demultiplexing residual pump light originating from the pumplight introduced into the one end of the rare earth doped fiber 1 by thefirst system and arriving at the other end of the rare earth doped fiber1 by a second optical coupler 3-2 and reflecting the demultiplexedresidual pump light by a reflection element (reflecting mirror) 4 so asto be introduced back into the rare earth doped fiber 1, and a thirdsystem for preventing the residual pump light introduced back into therare earth doped fiber 1 by the second system from being introduced intoa pump source 2, from which the pump light to be introduced into therare earth doped fiber 1 by the first system is produced, by an opticalisolation element (optical isolator) 5 so as to prevent unstableoperation of the pump source 2.

The reflection element 4 may be formed as a Faraday rotation reflectingmirror.

The optical fiber amplifier may further include an optical circulatorthrough which input signal light is inputted to the optical fiberamplifier and through which output signal light of the optical fiberamplifier is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 1 and including the rare earth doped fiber 1,pump source is introduced by way of the first optical coupler 3-1 intothe one end of the rare earth doped fiber 1, and residual pump lightoriginating from the pump light and arriving at the other end of therare earth doped fiber 1 is demultiplexed by the second optical coupler3-2. The residual pump light thus demultiplexed is reflected by thereflection element 4 (reflecting mirror 4: a Faraday rotation reflectingmirror can be used for the reflecting mirror 4) so that it is introducedback into the rare earth doped fiber 1.

If the residual pump light introduced back into the rare earth dopedfiber 1 is admitted, after passing the rare earth doped fiber 1, intothe pump source 2 for producing pump light to be introduced into therare earth doped fiber 1, then the pump source 2 operates but unstably.The optical isolation element 5 (optical isolator 5) intercepts theresidual pump light to prevent such unstable operation of the pumpsource 2.

Where the optical fiber amplifier includes the optical circulator, inputsignal light is inputted to the optical fiber amplifier and outputsignal light of the optical fiber amplifier is outputted both throughthe optical circulator.

Thus, with the optical fiber amplifier of the first aspect of thepresent invention, since the optical isolator 5 is interposed betweenthe pump source 2 and the first optical coupler 3-1 in order to preventunstable operation of the pump source 2 arising from interference of theresidual pump light introduced back into the rare earth doped fiber 1when the pump light is reflected by the reflecting mirror 4 so as to goback through the rare earth doped fiber 1, there is an advantage in thatthe optical fiber amplifier can make use of the pump power with a highefficiency while assuring stable operation of the pump source 2.

A2. Second Aspect of the Invention

Referring now to FIG. 2, there is shown in block diagram an opticalfiber amplifier according to a second aspect of the present invention.The optical fiber amplifier shown includes a first rare earth dopedfiber 11-1 and a second rare earth doped fiber 11-2 disposed at frontand rear stages.

The optical fiber amplifier further includes a pump source 12, a firstoptical coupler 13-1 provided at one end of one of the first rare earthdoped fiber 11-1 and the second rare earth doped fiber 11-2, that is, atone end of the rare earth doped fiber 11-1.

The optical fiber amplifier further includes a second optical coupler13-2 provided at the other end of the one rare earth doped fiber 11-1,and a third optical coupler 13-3 provided at one end of the other one ofthe first rare earth doped fiber 11-1 and the second rare earth dopedfiber 11-2, that is, at one end of the rare earth doped fiber 11-2.

The optical fiber amplifier further includes a reflecting mirror 14 forreflecting residual pump light demultiplexed by the second opticalcoupler 13-2 so as to be introduced back into the one rare earth dopedfiber 11-1 by way of the second optical coupler 13-2.

The optical fiber amplifier further includes an optical circulator 15having three or more ports connected to the pump source 12, the firstoptical coupler 13-1 and the third optical coupler 13-3.

In this instance, pump light from the pump source 12 is introduced intoone end of the one rare earth doped fiber 11-1 by way of the opticalcirculator 15 and the first optical coupler 13-1, and residual pumplight originating from the pump light introduced into the one end of theone rare earth doped fiber 11-1 and arriving at the other end of the onerare earth doped fiber 11-1 is demultiplexed by the second opticalcoupler 13-2 and reflected by the reflecting mirror 14 so as to beintroduced back into the one rare earth doped fiber 11-1. Thereafter,the residual pump light is introduced, after passing the one rare earthdoped fiber 11-1, into a different optical path by the opticalcirculator 15 so that the residual pump light is thereafter multiplexedwith an output of the other rare earth doped fiber 11-2 by the thirdoptical coupler 13-3.

In this instance, the optical fiber amplifier shown in FIG. 2 andincluding the first rare earth doped fiber 11-1 and the second rareearth doped fiber 11-2 disposed at front and rear stages is constructedsuch that it includes a first system for introducing pump light into theone end of the one rare earth doped fiber 11-1 by way of the opticalcirculator 15 having three or more ports and the first optical coupler13-1, a second system for demultiplexing residual pump light originatingfrom the pump light introduced into the one end of the one rare earthdoped fiber 11-1 by the first system and arriving at the other end ofthe one rare earth doped fiber 11-1 by the second optical coupler 13-2and reflecting the demultiplexed residual pump light by the reflectionelement 14 so as to be introduced back into the one rare earth dopedfiber 11-1, and a third system for causing the residual pump lightreflected from the reflection element 14 and introduced back into theone rare earth doped fiber 11-1 by the second system to follow, afterpassing the one rare earth doped fiber 11-1, the different optical pathby the optical circulator 15 and multiplexing the residual pump light Inthe different optical path with the output of the other rare earth dopedfiber 11-2 by the third optical coupler 13-3.

The optical fiber amplifier may further include an isolator provided atan input port of the optical fiber amplifier to which input signal lightis inputted, another isolator provided between an output of the secondoptical coupler 13-2 and an input of the third optical coupler 13-3, anda further isolator provided at an output port of the optical fiberamplifier from which output signal light is outputted (it is to be notedthat, where a pair of rare earth doped fibers are disposed at two frontand rear stages, it is very effective to additionally provide anisolator for both of the front and rear stages).

Also in this instance, the reflecting mirror 14 may be formed as aFaraday rotation reflecting mirror.

The optical fiber amplifier may further include an optical circulatorthrough which input signal light is inputted to the optical fiberamplifier and through which output signal light of the optical fiberamplifier is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 2 and including the first rare earth doped fiber11-1 and the second rare earth doped fiber 11-2 disposed at front andrear stages, pump light is introduced into the one end of the one rareearth doped fiber 11-1 by way of the optical circulator 15 and the firstoptical coupler 13-1 having three or more ports, and residual pump lightoriginating from the pump light introduced into the one end of the onerare earth doped fiber 11-1 and arriving at the other end of the onerare earth doped fiber 11-1 is demultiplexed by the second opticalcoupler 13-2 and reflected by the reflecting element 14 (reflectingmirror 14: a Faraday rotation reflecting mirror can be used for thereflecting mirror 14) so as to be introduced back into the one rareearth doped fiber 11-1.

Thereafter, the residual pump light is introduced, after passing the onerare earth doped fiber 11-1, into the different optical path by theoptical circulator 15 so that the residual pump light is thereaftermultiplexed with the output of the other rare earth doped fiber 11-2 bythe third optical coupler 13-3.

Where the optical fiber amplifier includes the additional isolators,input signal light is inputted by way of one of the isolators, and theinput signal light from the second optical coupler 13-2 is inputted tothe third optical coupler 13-3 by way of another one of the isolatorswhereas output signal light is outputted by way of the remainingisolator.

Where the optical fiber amplifier includes the optical circulator, inputsignal light is inputted to the optical fiber amplifier and outputsignal light of the optical fiber amplifier is outputted both throughthe optical circulator.

Thus, with the optical fiber amplifier of the second aspect of thepresent invention, since the optical amplifier including the first rareearth doped fiber 11-1 and the second rare earth doped fiber 11-2disposed at front and rear stages is constructed such that pump light isreflected by the reflecting mirror 14 so that it goes back through therare earth doped fiber 11-1 at the front stage and then is caused tofollow, after passing the rare earth doped fiber 11-1, the differentoptical path by the optical circulator 15 so that it is multiplexed withthe output of the other rare earth doped fiber 11-2 at the rear stage bythe third optical coupler 13-3, there is an advantage in that theoptical fiber amplifier of the two stage construction makes use of thepump power with a high efficiency.

A3. Third Aspect of the Invention

Referring now to FIG. 3, there is shown in block diagram an opticalfiber amplifier according to a third aspect of the present invention.The optical fiber amplifier shown includes a first rare earth dopedfiber 21-1 and a second rare earth doped fiber 21-2 disposed at frontand rear stages.

The optical fiber amplifier further includes a pump source 22, and anoptical branching element 23 for branching pump power from the pumpsource 22 at a ratio of n:1 (n is a real number equal to or greater than1).

The optical fiber amplifier further includes a first optical coupler24-1 for multiplexing pump light from a port of the optical branchingelement 23 and Introducing the multiplexed light into one of the firstrare earth doped fiber 21-1 and second rare earth doped fiber 21-2, thatis, into the rear earth doped fiber 21-1.

The optical fiber amplifier further includes a second optical coupler24-2 for extracting residual pump power outputted from the one rareearth doped fiber 21-1.

The optical fiber amplifier further includes a third optical coupler24-3 for multiplexing residual pump power extracted by the secondoptical coupler 24-2 and introducing the multiplexed power into theother one of the first rare earth doped fiber 21-1 and the second rareearth doped fiber 21-2, that is, into the rare earth doped fiber 21-2.

The optical fiber amplifier further includes a fourth optical coupler24-4 for multiplexing pump power from another port of the opticalbranching element 23 branched by the optical branching element 23 andintroducing the multiplexed power into the other rare earth doped fiber21-2.

In this instance, the optical fiber amplifier shown in FIG. 3 andincluding the first rare earth doped fiber 21-1 and the second rareearth doped fiber 21-2 disposed at front and rear stages is constructedsuch that it includes a first system for branching pump power at a ratioof n:1 (n is a real number equal to or greater than 1) by an opticalbranching element 23, multiplexing the pump light from a port of theoptical branching element 23 by a first optical coupler 24-1 andintroducing the multiplexed light into one end of the first rare earthdoped fiber 21-1, a second system for extracting residual pump poweroriginating from the pump light introduced into the one end of the onerare earth doped fiber by the first system and arriving at the other endof the one rare earth doped fiber by a second optical coupler 24-2connected to the other end of the one rare earth doped fiber,multiplexing the extracted residual pump power by a third opticalcoupler 24-3 and introducing the multiplexed power into one end of theother one of the first rare earth doped fiber 21-1 and the second rareearth doped fiber 21-2, and a third system for multiplexing the pumppower from another port of the optical branching element 23 branched bythe optical branching element 23 and introducing the multiplexed powerinto the other end of the other rare earth doped fiber 21-2 by a fourthoptical coupler 24-4.

The optical fiber amplifier may further include an isolator provided atan input port of the optical fiber amplifier to which input signal lightis inputted, another isolator provided between the pump source 22 andthe optical branching element 23, a further isolator provided betweenthe second optical coupler 24-2 and a signal port of the third opticalcoupler 24-3, and a still further isolator provided at an output port ofthe optical fiber amplifier from which output signal light is outputted.

Also here, the optical fiber amplifier may further include an opticalcirculator through which input signal light is inputted to the opticalfiber amplifier and through which output signal light of the opticalfiber amplifier is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 3 and including the first rare earth doped fiber21-1 and the second rare earth doped fiber 21-2 disposed at front andrear stages, pump power is branched at the ratio of n:1 (n is a realnumber equal to or greater than 1) by the optical branching element 23,and the pump light from a port of the optical branching element 23 ismultiplexed by the first optical coupler 24-1 and introduced into theone end of the one rare earth doped fiber 21-1.

Then, residual pump power originating from the pump light introducedinto the one end of the one rare earth doped fiber 21-1 and arriving atthe other end of the one rare earth doped fiber 21-1 is extracted by thesecond optical coupler 24-2 connected to the other end of the one rareearth doped fiber 21-1 and multiplexed by the third optical coupler24-3. Then, the thus multiplexed power is introduced into the one end ofthe other one rare earth doped fiber 21-2.

Further, the pump power from another port of the optical branchingelement 23 branched by the optical branching element 23 is multiplexedand introduced into the other end of the other rare earth doped fiber21-2 by the fourth optical coupler 24-4.

Where the optical fiber amplifier includes the additional isolators,input signal light is inputted by way of one of the isolators whereaspump light is inputted to the optical branching element 23 throughanother one of the isolators, and input signal light from the secondoptical coupler 24-2 is inputted to the third optical coupler 24-3 byway of a further one of the isolators whereas output light signal isoutputted through the remaining one of the isolators.

Also in this instance, where the optical fiber amplifier includes theoptical circulator, input signal light is inputted to the optical fiberamplifier and output signal light of the optical fiber amplifier isoutputted both through the optical circulator.

Thus, with the optical fiber amplifier of the third aspect of thepresent invention, since the optical amplifier of the two stageconstruction is constructed such that pump power is branched at theratio of n:1 and the pump light from a port of the optical branchingelement 23 is multiplexed by the first optical coupler 24-1 and thenintroduced into the one end of the rare earth doped fiber 21-1 at thefront stage or the rare earth doped fiber 21-2 at the rear stage whileresidual pump power is extracted by the second optical coupler 24-2connected to the other end of the rare earth doped fiber, whereafter theresidual pump power is multiplexed by the third optical coupler 24-3 andintroduced into the one end of the other rare earth doped fiber whilethe pump power from another port of the optical branching element 23branched by the optical branching element 23 is multiplexed andintroduced into the other end of the other rare earth doped fiber by thefourth optical coupler 24-4, there is an advantage in that the opticalfiber amplifier of the two stage construction makes use of the pumppower with a high efficiency.

A4. Fourth Aspect of the Invention

Referring now to FIG. 4, there is shown in block diagram an opticalfiber amplifier according to a fourth aspect of the present invention.The optical fiber amplifier shown includes a rare earth doped fiber 31,a pump source 32, and an optical circulator 33 having three or moreports one of which is connected to the pump source 32.

The optical fiber amplifier further includes a first optical coupler34-1 for multiplexing pump light introduced thereto from the pump source32 by way of the optical circulator 33 and introducing the multiplexedlight into one end of the rare earth doped fiber 31.

The optical fiber amplifier further includes a second optical coupler34-2 for demultiplexing residual pump light originating from pump lightintroduced into the one end of the rare earth doped fiber 31 by thefirst optical coupler 34-1 and arriving at the other end of the rareearth doped fiber 31.

The optical fiber amplifier further includes a reflecting mirror 35 forreflecting the residual pump light demultiplexed by the second opticalcoupler 34-2 so as to be introduced back into the rare earth doped fiber31 by way of the second optical coupler 34-2.

The optical fiber amplifier further includes a residual pump lightdetector 36 for detecting residual pump light introduced back into therare earth doped fiber 31 by the reflecting mirror 35 and inputted fromthe one end of the rare earth doped fiber 31 to the optical circulator33 by way of the first optical coupler 34-1.

The optical fiber amplifier further includes a controller 37 forcontrolling the pump source 32 so that residual pump light detected bythe residual pump light detector 36 may be constant.

Also in this instance, a Faraday rotation reflecting mirror can be usedfor the reflecting mirror 35.

Further, the optical fiber amplifier may further include an opticalcirculator through which input signal light is inputted to the opticalfiber amplifier and through which output signal light of the opticalfiber amplifier is outputted or may further include an isolator providedat an input port of the optical fiber amplifier to which input signallight is inputted and another isolator provided at an output port of theoptical fiber amplifier from which output signal light is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 4 and including the rare earth doped fiber 31,pump light is introduced into the one end of the rare earth doped fiber31 by way of the optical circulator 33 having three or more ports andthe first optical coupler 34-1, and residual pump light originating frompump light and arriving at the other end of the rare earth doped fiber31 is demultiplexed by the second optical coupler 34-2. Then, theresidual pump light is reflected by the reflecting mirror 35 (a Faradayrotation reflecting mirror can be used for the reflecting mirror 35) sothat It is introduced back into the rare earth doped fiber 31. Theresidual pump light is thereafter introduced, after passing the rareearth doped fiber 31, into a different optical path so that it isintroduced into the residual pump light detector 36. Thus, the pumpsource 32 is controlled by the controller 37 so that the residual pumplight detected by the residual pump light detector 36 may be constant.

Where the optical fiber amplifier includes the additional opticalcirculator, input signal light is inputted to the optical fiberamplifier and output signal light of the optical fiber amplifier isoutputted both through the optical circulator. On the other hand, wherethe optical fiber amplifier includes the additional isolators, inputsignal light is inputted through one of the isolators whereas outputsignal light is outputted through the other isolator.

Thus, with the optical fiber amplifier of the fourth aspect of thepresent invention, since residual pump power is extracted from thedifferent optical path to which it is introduced by the opticalcirculator 33 and is then monitored and controlled so as to be constant,the optical fiber amplifier is advantageous in that the wavelengthcharacteristic of the gain can be prevented from variation irrespectiveof a variation of the input level and this contributes very much torealization of a multiple wavelength collective amplifier.

A5. Fifth Aspect of the Invention

Referring now to FIG. 5, there is shown in block diagram an opticalfiber amplifier according to a fifth aspect of the present invention.The optical fiber amplifier shown includes a rare earth doped fiber 51and a dispersion compensating fiber 52 disposed at two front and rearstages.

The optical fiber amplifier further includes a first pump source 53-1for producing pump light of a first wavelength band for the rare earthdoped fiber 51, and a first optical coupler 54-1 for introducing thepump light from the first pump source 53-1 into the rare earth dopedfiber 51.

The optical fiber amplifier further includes a second pump source 53-2for producing pump light of a second wavelength band for the dispersioncompensating fiber 52, and a second optical coupler 54-2 for introducingthe pump light from the second pump source 53-2 into the dispersioncompensating fiber 52.

The dispersion compensating fiber 52 is pumped with pump light of thesecond wavelength band from the second Pump source 53-2 to cause Ramanamplification to occur.

In the optical fiber amplifier, a rare earth doped fiber opticalamplification element formed from the rare earth doped fiber 51 and aRaman optical amplification element formed from the dispersioncompensating fiber 52 which is pumped with pump light to cause Ramanamplification to occur are connected in cascade connection at two frontand rear stages.

Preferably, the wavelength band of the pump light produced by the firstpump source 53-1 is a 0.98 μm band while the wavelength band of the pumplight produced by the second pump source 53-2 is a 1.47 μm band (1.45 to1.49 μm: in the following description, unless otherwise specified, theterminology “1.47 μm band” signifies a band from 1.45 to 1.49 μm).

The Raman optical amplification element may be disposed as a front stageamplification element while the rare earth doped fiber opticalamplification element is disposed as a rear stage amplification element.Or, where the rare earth doped fiber optical amplification element isformed as an optical amplification element having a low noise figure,the rare earth doped fiber optical amplification element may be disposedas a front stage amplification element while the Raman opticalamplification element is disposed as a rear stage amplification element.

The second pump source 53-2 may include a pair of pump sources and apolarizing multiplexer for orthogonally polarizing and multiplexing pumplight from the pump sources or may include a combination of a pumpsource and a depolarizer by which pump light is depolarized or else mayproduce modulated pump light.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 5, pump light (whose wavelength band is, forexample, 0.98 μm) from the first pump source 53-1 is introduced into therare earth doped fiber 51 by way of the first optical coupler 54-1 whilepump light (whose wavelength band is, for example, 1.47 μm) from thesecond pump source 53-2 is introduced into the dispersion compensatingfiber 52 by way of the second optical coupler 54-2. Consequently, thedispersion compensating fiber 52 can be pumped with the pump light ofthe second wavelength band from the second pump source 53-2 to causeRaman amplification to occur.

Where the second pump source 53-2 includes the pair of pump sources andthe polarizing multiplexer, it supplies pump light obtained byorthogonal polarization and multiplexing of the pump light from the pumpsources. Meanwhile, where the second pump source 53-2 includes thecombination of the pump source and the depolarizer, it suppliesdepolarized pump light. On the other hand, where the second pump source53-2 produces modulated pump light, it supplies the modulated pumplight.

Thus, with the optical fiber amplifier of the fifth aspect of thepresent invention, since a rare earth doped fiber optical amplificationelement formed from the rare earth doped fiber 51 and a Raman opticalamplification element formed from the dispersion compensating fiber 52which is pumped with pump light to cause Raman amplification to occurare connected in cascade connection, there is an advantage in that theoptical fiber amplifier of the two stage construction makes use of thepump power with a high efficiency.

A6. Sixth Aspect of the Invention

Referring now to FIG. 6, there is shown in block diagram an opticalfiber amplifier according to a sixth aspect of the present invention.The optical fiber amplifier shown includes an erbium-doped-fiber 61 anda dispersion compensating fiber 62 disposed at two front and rearstages.

The optical fiber amplifier further includes a pump source 63 forproducing pump light of the 1.47 μm band, and an optical coupler 64 forintroducing the pump light from the pump source 63 into theerbium-doped-fiber 61.

Here, the dispersion compensating fiber 62 is pumped with residual pumplight from the erbium-doped-fiber 61 to cause Raman amplification tooccur.

In the optical fiber amplifier, a rare earth doped fiber opticalamplification element formed from the erbium-doped-fiber 61 which is arare earth doped fiber and a Raman optical amplification element (whichis formed from the dispersion compensating fiber 62) which is pumpedwith pump light, which is capable of pumping the rare earth doped fiberoptical amplification element, to cause Raman amplification to occur areconnected in cascade connection, and the pump source 63 for supplyingpump light for pumping the rare earth doped fiber optical amplificationelement and the Raman optical amplification element is provided.

The pump source 63 may include a pair of pump sources and a polarizingmultiplexer for orthogonally polarizing and multiplexing pump light fromthe pump sources or may include a combination of a pump source and adepolarizer by which pump light is depolarized or else may producemodulated pump light.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 6, the erbium-doped-fiber 61 is pumped with pumplight of the 1.47 μm band whereas the dispersion compensating fiber 62is pumped with residual pump light from the erbium-doped-fiber 61 tocause Raman amplification to occur.

Where the pump source 63 includes the pair of pump sources and thepolarizing multiplexer, it supplies pump light obtained by orthogonalpolarization and multiplexing of the pump light from the pump sources.Meanwhile, where the pump source 63 includes the combination of the pumpsource and the depolarizer, it supplies depolarized pump light. On theother hand, where the pump source 63 produces modulated pump light, itsupplies the modulated pump light.

Thus, with the optical fiber amplifier of the sixth aspect of thepresent invention, since the common pump source for supplying pump lightfor pumping the rare earth doped fiber optical amplification element andthe Raman optical amplification element is provided, the optical fiberamplifier can make use of the pump power with a high efficiency, and thenumber of pump sources to be used can be reduced, which contributes tosimplification in construction and reduction in cost.

A7. Seventh Aspect of the Invention

Referring now to FIG. 7, there is shown in block diagram an opticalfiber amplifier according to a seventh aspect of the present invention.The optical fiber amplifier shown includes an erbium-doped-fiber 71 anda dispersion compensating fiber 72 disposed at two front and rearstages.

The optical fiber amplifier further includes a pump source 73 forproducing pump light of the 1.47 μm band, and an optical coupler 74 forintroducing the pump light from the pump source 73 into the dispersioncompensating fiber 72.

In this instance, the erbium-doped-fiber 71 is pumped with residual pumplight from the dispersion compensating fiber 72.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 7, the dispersion compensating fiber 72 is causedto perform Raman amplification using pump light of the 1.47 μm bandwhereas the erbium-doped-fiber 71 is pumped with residual pump lightfrom the dispersion compensating fiber 72.

Thus, with the optical fiber amplifier of the seventh aspect of thepresent invention, since the common pump source for supplying pump lightfor pumping the erbium-doped-fiber 71 and the dispersion compensatingfiber 72 is provided, the optical fiber amplifier can make use of thepump power with a high efficiency, and the number of pump sources to beused can be reduced, which contributes to simplification in constructionand reduction in cost.

A8. Eighth Aspect of the Invention

Referring now to FIG. 8, there is shown in block diagram an opticalfiber amplifier according to an eighth aspect of the present invention.The optical fiber amplifier shown includes a dispersion compensatingfiber (rare earth doped dispersion compensating fiber) 81 doped with arare earth element, a pump source 82 for producing pump light for therare earth doped dispersion compensating fiber 81, and an opticalcoupler 83 for introducing the pump light from the pump source 82 intothe rare earth doped dispersion compensating fiber 81.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 8, pump light from the pump source 82 isintroduced into the the rare earth doped dispersion compensating fiber81 doped with a rare earth element to pump the rare earth dopeddispersion compensating fiber 81.

Thus, with the optical fiber amplifier of the eighth aspect of thepresent invention, since the dispersion compensating fiber is doped witha rare earth element, the loss of the dispersion compensating fiber isreduced while dispersion compensation is performed. Further, the opticalfiber amplifier with a dispersion compensating function can opticallyamplify signal light sufficiently.

A9. Ninth Aspect of the Invention

Referring now to FIG. 9, there is shown in block diagram an opticalfiber amplifier according to a ninth aspect of the present invention.The optical fiber amplifier shown includes an erbium-doped-fiber 91 anda dispersion compensating fiber 92 disposed at two front and rearstages.

The optical fiber amplifier further includes a pump source 93 forproducing pump light of the 1.47 μm band for the erbium-doped-fiber 91,and an optical coupler 94 for introducing the pump light from the pumpsource 93 into the erbium-doped-fiber 91.

The optical fiber amplifier further includes an optical filter 95interposed between the erbium-doped-fiber 91 and the dispersioncompensating fiber 92 for intercepting residual pump light of the 1.47μband coming out from the erbium-doped-fiber 91.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 9, the erbium-doped-fiber 91 is pumped with pumplight of the 1.47 μm band from the pump source 93. In this instance,residual pump light of the 1.47 μm band coming out from theerbium-doped-fiber 91 is intercepted by the optical filter 95 so that itis prevented from being Inputted to the dispersion compensating fiber92.

Thus, with the optical fiber amplifier of the ninth aspect of thepresent invention, since the optical filter 95 which prevents pump lightof the 1.47 μm band from being inputted to the dispersion compensatingfiber 92 is provided, leaking pump power of the 1.47 μm band causes thedispersion compensating fiber 92 to perform Raman amplification, andconsequently, the optical fiber amplifier can be prevented from unstableoperation or from variation of the wavelength dependency of theamplification band.

A10. Tenth Aspect of the Invention

Referring now to FIG. 10( a), there is shown in block diagram an opticalfiber amplifier according to a tenth aspect of the present invention.The optical fiber amplifier shown includes a silica-type-optical-fiber(SOF) 101 and an erbium-doped-fiber (EDF) 102. In the optical fiberamplifier shown in FIG. 10( a), the silica-type-optical-fiber 101 andthe erbium-doped-fiber 102 are provided at a front stage and a rearstage, respectively.

The optical fiber amplifier further includes a silica-type-optical-fiberpump source 103-1 for producing pump light of a wavelength band for thesilica-type-optical-fiber 101, and an optical coupler 104-1 forintroducing the pump light from the silica-type-optical-fiber pumpsource 103-1 into the silica-type-optical-fiber 101.

The optical fiber amplifier further includes an erbium-doped-fiber pumpsource 103-2 for producing pump light of a wavelength band for theerbium-doped-fiber 102, and another optical coupler 104-2 forintroducing the pump light from the erbium-doped-fiber pump source 103-2into the erbium-doped-fiber 102;

In this instance, the silica-type-optical-fiber 101 is pumped with thepump light from the silica-type-optical-fiber pump source 103-1 to causeRaman amplification to occur.

In particular, in the optical fiber amplifier shown in FIG. 10( a), arare earth doped fiber optical amplification element formed from theerbium-doped-fiber 102 which is a rare earth doped fiber and a Ramanoptical amplification element formed from the silica-type-optical-fiber101 which causes, when pumped with pump light, Raman amplification tooccur are connected in cascade connection at two front and rear stages.Further, the Raman optical amplification element is disposed as a frontstage amplification element while the rare earth doped fiber opticalamplification element is disposed as a rear stage amplification element.

Where the rare earth doped fiber optical amplification element is formedas an optical amplification element having a low noise figure, the rareearth doped fiber optical amplification element may be disposed as afront stage amplification element while the Raman optical amplificationelement is disposed as a rear stage amplification element.

Further, the optical fiber amplifier may additionally include a pumpsource which produces pump light and serves both as thesilica-type-optical-fiber pump source 103-1 and the erbium-doped-fiberpump source 103-2.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 10( a), pump light from thesilica-type-optical-fiber pump source 103-1 is introduced into thesilica-type-optical-fiber 101 by way of the optical coupler 104-1 whilepump light from the erbium-doped-fiber pump source 103-2 is introducedinto the erbium-doped-fiber 102 by way of the optical coupler 104-2.Consequently, the silica-type-optical-fiber 101 can be pumped with thepump light of the wavelength band therefor from thesilica-type-optical-fiber pump source 103-1 to cause Raman amplificationto occur.

Thus, with the optical fiber amplifier of the tenth aspect of thepresent invention, since the optical fiber amplifier includes the Ramanoptical amplification element formed from the silica-type-optical-fiber101 and causes, when pumped with pump light, Raman amplification tooccur and the rare earth doped fiber optical amplification elementformed from the erbium-doped-fiber 102 are connected in cascadeconnection, there is an advantage in that the optical fiber amplifier ofthe two stage construction makes use of the pump power with a highefficiency.

Further, where the rare earth doped fiber optical amplification elementis formed as an optical amplification element having a low noise figureand is disposed as a front stage amplification element while the Ramanoptical amplification element is disposed as a rear stage amplificationelement, there is an advantage in that the optical fiber amplifier ofthe two stage construction makes use of the pump power with a highefficiency.

Furthermore, where the optical fiber amplifier additionally includes thepump source which produces pump light for pumping both of the Ramanoptical amplification element and the rare earth doped fiber opticalamplification element is provided, the optical fiber amplifier can makeuse of the pump power with a high efficiency, and the number of pumpsources to be used can be reduced, which contributes to simplificationin construction and reduction in cost.

A11. Eleventh Aspect of the Invention

Referring now to FIG. 10( b), there is shown in block diagram an opticalfiber amplifier according to an eleventh aspect of the presentinvention. The optical fiber amplifier shown includes anerbium-doped-fiber (EDF) 111 having a low noise figure and asilica-type-optical-fiber (SOF) 112. In the optical fiber amplifiershown in FIG. 10( b), the erbium-doped-fiber 111 and thesilica-type-optical-fiber (SOF) 112 are provided at a front stage and arear stage, respectively.

The optical fiber amplifier further includes a silica-type-optical-fiberpump source 113-2 for producing pump light of a wavelength band for thesilica-type-optical-fiber 112, and an optical coupler 114-2 forintroducing the pump light from the silica-type-optical-fiber pumpsource 113-2 into the silica-type-optical-fiber 112.

The optical fiber amplifier further includes an erbium-doped-fiber pumpsource 113-1 for producing pump light of a wavelength band for theerbium-doped-fiber 111, and another optical coupler 114-1 forintroducing the pump light from the erbium-doped-fiber pump source 113-1into the erbium-doped-fiber 111.

In this instance, the silica-type-optical-fiber 112 is pumped with pumplight from the silica-type-optical-fiber pump source 113-2 to causeRaman amplification to occur.

The optical fiber amplifier may further include a pump source whichproduces pump light of the 1.47 μm band and serves both as thesilica-type-optical-fiber pump source 113-2 and the erbium-doped-fiberpump source 113-1.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 10( b), pump light from the erbium-doped-fiberpump source 113-1 is introduced into the erbium-doped-fiber 111 by wayof the optical coupler 114-1 while pump light from thesilica-type-optical-fiber pump source 113-2 is introduced into thesilica-type-optical-fiber 112 by way of the optical coupler 114-2.Consequently, the silica-type-optical-fiber 112 can be pumped with thepump light of the wavelength band therefor from thesilica-type-optical-fiber pump source 113-2 to cause Raman amplificationto occur.

Thus, with the optical fiber amplifier of the eleventh aspect of thepresent invention, since the optical fiber amplifier includes a Ramanoptical amplification element formed from the silica-type-optical-fiber112 for causing, when pumped with pump light, Raman amplification tooccur and a rare earth doped fiber optical amplification element formedfrom the erbium-doped-fiber 111 and arranged in tandem to the Ramanoptical amplification element, there is an advantage in that the opticalfiber amplifier of the two stage construction makes use of the pumppower with a high efficiency.

Further, where the optical fiber amplifier additionally includes thepump source which supplies pump light for pumping both of the Ramanoptical amplification element and the rare earth doped fiber opticalamplification element is provided, the optical fiber amplifier can makeuse of the pump power with a high efficiency, and the number of pumpsources to be used can be reduced, which contributes to simplificationin construction and reduction in cost.

A12. Twelfth Aspect of the Invention

Referring now to FIG. 11, there is shown in block diagram an opticalfiber amplifier according to a twelfth aspect of the present invention.The optical fiber amplifier shown includes a first erbium-doped-fiber(EDF) 121-1 having a low noise figure, a silica-type-optical-fiber (SOF)122 and a second erbium-doped-fiber (EDF) 121-2. In the optical fiberamplifier shown in FIG. 11, the first erbium-doped-fiber 121-1, thesilica-type-optical-fiber 122 and the second erbium-doped-fiber 121-2are provided at a front stage, a middle stage and a rear stage,respectively.

The optical fiber amplifier further includes a first erbium-doped-fiberpump source 123-1 for producing pump light of a wavelength band for thefirst erbium-doped-fiber 121-1, and an optical coupler 124-1 forintroducing the pump light from the first erbium-doped-fiber pump source123-1 into the first erbium-doped-fiber 121-1.

The optical fiber amplifier further includes a silica-type-optical-fiberpump source 123-2 for producing pump light of a wavelength band for thesilica-type-optical-fiber 122, and another optical coupler 124-2 forintroducing the pump light from the silica-type-optical-fiber pumpsource 123-2 into the silica-type-optical-fiber 122.

The optical fiber amplifier further includes a second erbium-doped-fiberpump source 123-3 for producing pump light of a wavelength band for thesecond erbium-doped-fiber 121-2, and a further optical coupler 124-3 forintroducing the pump light from the second erbium-doped-fiber pumpsource 123-3 into the second erbium-doped-fiber 121-2.

In this instance, the silica-type-optical-fiber 122 is pumped with thepump light from the silica-type-optical-fiber pump source 123-2 to causeRaman amplification to occur.

In the optical fiber amplifier shown in FIG. 11, a rare earth dopedfiber optical amplification element formed from the erbium-doped-fiber121-1 which is a rare earth doped fiber and having a low noise figure isdisposed as a front stage amplification element; a Raman opticalamplification element formed from the silica-type-optical-fiber 122 forcausing Raman amplification to occur when pumped with pump light isdisposed as a middle stage amplification element; and another rare earthdoped fiber optical amplification element formed from theerbium-doped-fiber 121-2 which is a rare earth doped fiber is disposedas a rear stage amplification element.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 11, pump light from the first erbium-doped-fiberpump source 123-1 is introduced into the first erbium-doped-fiber 121-1by way of the optical coupler 124-1 and pump light from thesilica-type-optical-fiber pump source 123-2 is introduced into thesilica-type-optical-fiber 122 by way of the optical coupler 124-2 whilepump light from the second erbium-doped-fiber pump source 123-3 isintroduced into the second erbium-doped-fiber 121-2 by way of theoptical coupler 124-3.

Consequently, the silica-type-optical-fiber 122 can be pumped with thepump light of the wavelength band therefor from thesilica-type-optical-fiber pump source 123-2 to cause Raman amplificationto occur.

Thus, with the optical fiber amplifier of the twelfth aspect of thepresent invention, since the first erbium-doped-fiber 121-1 having a lownoise figure, the silica-type-optical-fiber 122 and the seconderbium-doped-fiber 121-2 are provided at the front stage, the middlestage and the rear stages respectively, such that residual pump lightfrom the first and second erbium-doped-fibers 121-1 and 121-2 positionedon the front and the rear to the silica-type-optical-fiber 122 are usedfor Raman amplification of the silica-type-optical-fiber 122, thesilica-type-optical-fiber 122 exhibits an improved compensation effect.Consequently, a wide bandwidth optical amplifier can be realized whileachieving simplification in structure and reduction in cost.

A13. Thirteenth Aspect of the Invention

Referring now to FIG. 12, there is shown in block diagram an opticalfiber amplifier according to a thirteenth aspect of the presentinvention. The optical fiber amplifier shown includes a firsterbium-doped-fiber (EDF) 131-1 having a low noise figure, a dispersioncompensating fiber (DCF) 132 and a second erbium-doped-fiber (EDF)131-2. In the optical fiber amplifier shown in FIG. 12, the firsterbium-doped-fiber 131-1, the dispersion compensating fiber 132 and thesecond erbium-doped-fiber 131-2 art provided at a front stage, a middlestage and a rear stage, respectively.

The optical fiber amplifier further includes a first erbium-doped-fiberpump source 133-1 for producing pump light of a wavelength band for thefirst erbium-doped-fiber 131-1, and an optical coupler 134-1 forIntroducing the pump light from the first erbium-doped-fiber pump source133-1 into the first erbium-doped-fiber 131-1.

The optical fiber amplifier further includes a dispersion compensatingfiber pump source 133-2 for producing pump light of a wavelength bandfor the dispersion compensating fiber 132, and another optical coupler134-2 for introducing the pump light from the dispersion compensatingfiber pump source 133-2 into the dispersion compensating fiber 132.

The optical fiber amplifier further includes a second erbium-doped-fiberpump source 133-3 for producing pump light of a wavelength band for thesecond erbium-doped-fiber 131-2, and a further optical coupler 134-3 forintroducing the pump light from the second erbium-doped-fiber pumpsource 133-3 into the second erbium-doped-fiber 131-2.

In this instance, the dispersion compensating fiber 132 is pumped withthe pump light from the dispersion compensating fiber pump source 133-2to cause Raman amplification to occur.

In the optical fiber amplifier shown in FIG. 12, a rare earth dopedfiber optical amplification element formed from the erbium-doped-fiber131-1 which is a rare earth doped fiber and having a low noise figure isdisposed as a front stage amplification element; a Raman opticalamplification element formed from the dispersion compensating fiber 132for causing Raman amplification to occur when pumped with pump light isdisposed as a middle stage amplification element; and another rare earthdoped fiber optical amplification element formed from theerbium-doped-fiber 131-2 which is a rare earth doped fiber is disposedas a rear stage amplification element.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 12, pump light from the first erbium-doped-fiberpump source 133-1 is introduced into the first erbium-doped-fiber 131-1by way of the optical coupler 134-1 and pump light from the dispersioncompensating fiber pump source 133-2 is introduced into the dispersioncompensating fiber 132 by way of the optical coupler 134-2 while pumplight from the second erbium-doped-fiber pump source 133-3 is Introducedinto the second erbium-doped-fiber 131-2 by way of the optical coupler134-3.

Consequently, the dispersion compensating fiber 132 can be pumped withthe pump light of the wavelength band therefor from the dispersioncompensating fiber pump source 133-2 to cause Raman amplification tooccur.

Thus, with the optical fiber amplifier of the thirteenth aspect of thepresent invention, since the first erbium-doped-fiber 131-1 having a lownoise figure, the dispersion compensating fiber 132 and the seconderbium-doped-fiber 131-2 are provided at the front stage, the middlestage and the rear stage, respectively, such that residual pump lightfrom the first and second erbium-doped-fibers 131-1 and 131-2 positionedon the front and the rear to the dispersion compensating fiber 132 areused for Raman amplification of the dispersion compensating fiber 132,the dispersion compensating fiber 132 exhibits an improved compensationeffect. Consequently, a wide bandwidth optical amplifier can be realizedwhile achieving simplification in structure and reduction in cost.

A14. Fourteenth Aspect of the Invention

Referring now to FIG. 13( a), there is shown in block diagram an opticalfiber amplifier according to a fourteenth aspect of the presentinvention. The optical fiber amplifier shown includes a dispersioncompensating fiber (DCF) 141, a pump source 142 for producing pumplight, and an optical coupler 143 for introducing pump light from thepump source 142 into the dispersion compensating fiber 141. Thedispersion compensating fiber 141 is pumped with pump light from thepump source 142 to cause Raman amplification to occur.

Accordingly, the optical fiber amplifier includes a dispersioncompensating fiber module which includes the dispersion compensatingfiber 141, and the pump source 142 for pumping the dispersioncompensating fiber 141 to cause Raman amplification to occur.

Also in this instance, the optical fiber amplifier may further includean optical circulator through which input signal light is inputted tothe optical fiber amplifier and through which output signal light of theoptical fiber amplifier is outputted, or may additionally include anisolator provided at an input port of the optical fiber amplifier towhich input signal light is inputted and/or another isolator provided atan output port of the optical fiber amplifier from which output signallight is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 13( a), the dispersion compensating fiber 141 ispumped with pump light from the pump source 142 to cause Ramanamplification to occur.

Where the optical fiber amplifier includes the additional opticalcirculator, input signal light is inputted to the optical fiberamplifier and output signal light of the optical fiber amplifier isoutputted both through the optical circulator. On the other hand, wherethe optical fiber amplifier includes the additional isolators, inputsignal light is inputted through one of the isolators whereas outputsignal light is outputted through the other isolator.

Thus, with the optical fiber amplifier of the fourteenth aspect of thepresent invention, since it is constructed using the module wherein thedispersion compensating fiber 141 is pumped to cause Raman amplificationto occur, there is an advantage in that the loss of the dispersioncompensating fiber 141 can be reduced.

Also in this instance, where the additional circulators are provided atthe input and output portions of the optical fiber amplifier, the numberof isolators to be used can be reduced, which contributes to reductionin cost.

A15. Fifteenth Aspect of the Invention

Referring now to FIG. 13( b), there is shown in block diagram an opticalfiber amplifier according to a fifteenth aspect of the presentinvention. The optical fiber amplifier shown includes asilica-type-optical-fiber (SOF) 151, a pump source 152 for producingpump light, and an optical coupler 153 for introducing the pump lightfrom the pump source 152 into the silica-type-optical-fiber 151. Thesilica-type-optical-fiber 151 is pumped with the pump light from thepump source 152 to cause Raman amplification to occur.

Also in this instance, the optical fiber amplifier may further includesan optical circulator through which input signal light is inputted tothe optical fiber amplifier and through which output signal light of theoptical fiber amplifier is outputted.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 13( b), the silica-type-optical-fiber 151 ispumped with pump light from the pump source 152 to cause Ramanamplification to occur.

Also here, where the optical fiber amplifier includes the additionaloptical circulator, input signal light is inputted to the optical fiberamplifier and output signal light of the optical fiber amplifier isoutputted both through the optical circulator. On the other hand, wherethe optical fiber amplifier includes the additional isolators, inputsignal light is inputted through one of the isolators whereas outputsignal light is outputted through the other isolator.

Thus, with the optical fiber amplifier of the fifteenth aspect of thepresent invention, since the silica-type-optical-fiber 151 is pumped tocause Raman amplification to occur, there is an advantage in that theloss of the silica-type-optical-fiber 151 can be reduced.

Also in this instance, where the additional circulators are provided atthe input and output portions of the optical fiber amplifier, the numberof isolators to be used can be reduced, which contributes to reductionin cost.

A16. Sixteenth Aspect of the Invention

Referring now to FIG. 14, there is shown in block diagram an opticalfiber amplifier according to a sixteenth aspect of the presentinvention. The optical fiber amplifier shown includes a rare earth dopedfiber optical amplification element 154 formed from a rare earth dopedfiber 61, and an optical fiber attenuation element 155 formed from anoptical fiber or an optical fiber with an optical isolator.

The optical fiber attenuation element 155 suppresses unstable operationof the rare earth doped fiber optical amplification element 154.

The optical fiber attenuation element 155 may serve also as a Ramanoptical amplification element which is pumped with pump light to causeRaman amplification to occur.

It is to be noted that, in FIG. 14, reference numeral 63 denotes a pumpsource, and 64 an optical coupler which introduces pump light from thepump source 63 into the rare earth doped fiber 61.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 14, when the erbium-doped-fiber 61 is pumped withpump light from the pump source 63 in the rare earth doped fiber opticalamplification element 154, if the rare earth doped fiber opticalamplification element 154 operates unstably, the optical fiberattenuation element 155 suppresses the unstable operation of the rareearth doped fiber optical amplification element 154.

The optical fiber attenuation element 155 may be pumped with residualpump light from the erbium-doped-fiber 61 to cause Raman amplificationto occur.

In this manner, due to the provision of the optical fiber attenuationelement 155, unstable operation of the rare earth doped fiber opticalamplification element 154 can be suppressed so that stabilized opticalamplification of the optical fiber amplifier can be achieved.

A17. Seventeenth Aspect of the Invention

Referring now to FIG. 15, there is shown in block diagram an opticalfiber amplifier according to a seventeenth aspect of the presentinvention. The optical fiber amplifier shown includes a front stageoptical amplification element 156-1 and a rear stage opticalamplification element 156-2 each formed as a rare earth doped fiberoptical amplification element formed from a rare earth doped fiber 121-1or 121-2. The front stage optical amplification element 156-1 and therear stage optical amplification element 156-2 form an opticalamplification unit.

The optical fiber amplifier further includes an optical fiberattenuation element 157 formed from an optical fiber or an optical fiberwith an optical Isolator interposed between the front stage opticalamplification element 156-1 and the rear stage optical amplificationelement 156-2 of the optical amplification unit. The optical fiberattenuation element 157 suppresses unstable operation of the opticalamplification unit.

The optical fiber attenuation element 157 may serve also as a Ramanoptical amplification element which is pumped with pump light to causeRaman amplification to occur.

It is to be noted that, in FIG. 15, reference numerals 123-1 and 123-3denote each a pump source, and reference numeral 124-1 denotes anoptical coupler for introducing pump light from the pump source 123-1into the rare earth doped fiber 121-1, and 124-3 an optical coupler forintroducing pump light from the pump source 123-3 into the rare earthdoped fiber 121-2.

In the optical fiber amplifier having the construction described abovewith reference to FIG. 15, when the erbium-doped-fiber 121-1 is pumpedwith pump light from the pump source 123-1 in the front stage opticalamplification element 156-1 in the optical amplification unit and theerbium-doped-fiber 121-2 is pumped with pump light from the pump source123-3 in the rear stage optical amplification element 156-2 in theoptical amplification unit, if the front stage optical amplificationelement 156-1 and the rear stage optical amplification element 156-2 inthe optical amplification unit operate unstably, the optical fiberattenuation element 157 suppresses the unstable operation of the frontstage optical amplification element 156-1 and the rear stage opticalamplification element 156-2 in the optical amplification unit.

The optical fiber attenuation element 157 may be pumped with residualpump light from the erbium-doped-fibers 121-1 and 121-2 to cause Ramanamplification to occur.

In this manner, since the optical fiber attenuation element 157 isinterposed between the front stage optical amplification element 156-1and the rear stage optical amplification element 156-2 in the opticalamplification unit, unstable operation of the front stage opticalamplification element 156-1 and the rear stage optical amplificationelement 156-2 in the optical amplification unit can be suppressed toachieve stabilized optical amplification of the optical fiber amplifier.

B. Preferred Embodiments of the Invention

The present invention will be described in more detail below inconnection with preferred embodiments thereof shown in the accompanyingdrawings.

B1. First Embodiment

Referring now to FIG. 16, there is shown in block diagram an opticalfiber amplifier according to a first preferred embodiment of the presentinvention. The optical fiber amplifier shown includes a pair oferbium-doped-fibers (EDF) 11-1 and 11-2 each as a rare earth dopedfiber, a pair of pump sources 12-1 and 12-2, four opticaldemultiplexer-multiplexers (WDM; optical wave separator-combiners) 13-1to 13-4 serving as first to fourth optical couplers, respectively, areflecting mirror (reflection element) 14, an optical circulator 15,three isolators (ISO) 16-1 to 16-3, and an optical filter 17.

In particular, in the optical fiber amplifier, the isolator 16-1,optical demultiplexer-multiplexer 13-1, erbium-doped-fiber 11-1, opticaldemultiplexer-multiplexer 13-2, optical filter 17, isolator 16-2,optical demultiplexer-multiplexer 13-3, erbium-doped-fiber 11-2, opticaldemultiplexer-multiplexer 13-4 and isolator 16-3 are arranged in thisorder from the input side.

The pump source 12-1 is connected to the opticaldemultiplexer-multiplexer 13-1 by way of the optical circulator 15. Theoptical circulator 15 is connected, in addition to the pump source 12-1,at another port thereof to the optical demultiplexer-multiplexer 13-3.Meanwhile, the reflecting mirror 14 is connected to the opticaldemultiplexer-multiplexer 13-2. It is to be noted that the pump source12-2 is connected to the optical demultiplexer-multiplexer 13-4.

Each of the erbium-doped-fibers 11-1 and 11-2 functions as an opticalamplification element. The pump source 12-1 is formed from a lens and anLD chip and serves as a pump source which produces pump light of, forexample, the 0.98 μm band. Meanwhile, the pump source 12-2 is formedfrom a pair of lenses, an optical isolator (optical ISO) and an LD chipand serves as a pump source which produces pump light of, for example,the 1.47 μm band (the terminology “1.47 μm band” signifies, in thefollowing description of the various embodiments, a band ranging from1.45 to 1.49 μm in wavelength). It is to be noted that the reason whythe pump source 12-2 which produces pump light of the 1.47 μm bandincludes a built-in optical isolator (optical ISO) is that it isintended to prevent noise light of the 1.55 μm band generated in theerbium-doped-fiber 11-2 upon amplification of an optical signal of the1.55 μm band from returning to the pump source 12-2.

Where the pump light wavelengths of the pump sources 12-1 and 12-2 areselected in such a manner as described above, an opticaldemultiplexer-multiplexer of the 0.98 μm band is used for the opticaldemultiplexer-multiplexers 13-1 to 13-3, and another opticaldemultiplexer-multiplexer of the 1.47 bandwidth is used for the opticaldemultiplexer-multiplexer 13-4.

Further, while, in the arrangement shown in FIG. 16, an opticaldemultiplexer-multiplexer of the fusion type is used for the opticaldemultiplexer-multiplexers 13-1 to 13-4, naturally another opticaldemultiplexer-multiplexer of the bulk (dielectric multi-layer film) typemay be employed alternatively. Where, for example, an opticaldemultiplexer-multiplexer of the bulk type is employed for the opticaldemultiplexer-multiplexer 13-4, the optical isolator (optical ISO) buildin the pump source 12-2 can be omitted, and consequently, a pump sourceof the same type as that of the pump source 12-1 (but of the 1.47 μmband) is employed for the pump source 12-2 (this similarly applies tothe other embodiments hereinafter described).

Meanwhile, a Faraday rotation reflecting mirror is employed for thereflecting mirror 14. Thus, residual pump light demultiplexed by theoptical demultiplexer-multiplexer 13-2 is reflected using the reflectingmirror 14 so that it may be introduced back into the erbium-doped-fiber11-1 by way of the optical demultiplexer-multiplexer 13-2.

An optical circulator of the three port type is used for the opticalcirculator 15. Accordingly, the optical circulator 15 is constructedequivalently to an optical circulator of the four port type shown inFIG. 53 which has no fiber connected to a port 4 thereof.

As seen in FIG. 16, the pump source 12-1 is connected to a port 1 of theoptical circulator 15: the optical demultiplexer-multiplexer 13-1 isconnected to another port 2 of the optical circulator 15; and theoptical demultiplexer-multiplexer 13-3 is connected to the other port 3of the optical circulator 15.

It is to be noted that the optical circulator 15 may alternatively beconstructed as an optical circulator having more than three ports.

The isolators 16-1 to 16-3 allow light to pass therethrough only in thedirections indicated by respective arrow marks. As seen in FIGS. 54( a)and 54(b), each of the isolators 16-1 to 16-3 includes a lens, a pair ofbirefringent prisms A and B, a polarizing rotator (reciprocal) and a45-degree Faraday rotator (non-reciprocal).

When an optical signal is inputted from a fiber on the left side in FIG.54( a) to any of the isolators 16-1 to 16-3, the optical signal arrivesat another fiber on the right side through the optical isolator as seenin FIG. 54( a). However, even if an optical signal is inputted from thefiber on the right side, it does not arrive at the fiber on the leftside as seen from FIG. 54( b) (In the embodiments described below,unless otherwise specified, each isolator has the structure illustratedin FIGS. 54( a) and 54(b)).

Referring back to FIG. 16, in the optical fiber amplifier of the presentembodiment, the isolators 16-1 and 16-2 are disposed at the front andrear stages to the erbium-doped-fiber 11-1, respectively, and theisolators 16-2 and 16-3 are disposed at the front and rear stages to theerbium-doped-fiber 11-2, respectively, so that production of noise lightin the erbium-doped-fibers 11-1 and 11-2 is prevented.

It is to be noted that, in an optical amplifier which includes aplurality of optical amplification elements, it is particularlyimportant to prevent production of noise light by the erbium-doped-fiber11-1 which is an amplification element positioned on the input side ofan optical signal in order to amplify light with low noise production,and accordingly, the isolator 16-3 at the rear stage to theerbium-doped-fiber 11-2 which is an amplification element positioned onthe output side of an optical signal can be omitted (this similarlyapplies to the other embodiments hereinafter described).

The optical filter 17 cuts a mountain-like portion of the outputcharacteristic of ASE (Amplified Spontaneous Emission) of theerbium-doped-fiber 11-1 (for example, a portion at 1.535 μm; refer toFIG. 46) (that is, levels the mountain into a flat shape or cuts awaythe shorter wavelength side than 1.538 μm). The optical filter 17includes a dielectric multi-layer film. The optical filter 17, however,may be omitted.

In the optical fiber amplifier having the construction described above,pump light from the pump source 12-1 first passes through the opticalcirculator 15 and is then multiplexed with signal light from theisolator 16-1 by the optical demultiplexer-multiplexer 13-1, and thethus multiplexed light is introduced into one end of theerbium-doped-fiber 11-1. Consequently, optical amplification isperformed by the erbium-doped-fiber 11-1. In this instance, since theerbium-doped-fiber 11-1 has a comparatively small length so as to assurea high average pump ratio, residual pump power leaks out from the otherend of the erbium-doped-fiber 11-1.

The residual pump light arriving at and leaking out from the other endof the erbium-doped-fiber 11-1 in this manner is demultiplexed from thesignal light by the optical demultiplexer-multiplexer 13-2 and thenreflected by the reflecting mirror 14 backwardly.

Thereafter, the reflected residual pump light is introduced into theerbium-doped-fiber 11-1 and passed on to the optical circulator 15 byway of the optical demultiplexer-multiplexer 13-1. By the opticalcirculator 15, the reflected residual pump light now is introduced intoa different optical path so that it is introduced into the opticaldemultiplexer-multiplexer 13-3. Consequently, the residual pump light ismultiplexed by the optical demultiplexer-multiplexer 13-3 with thesignal light from the isolator 16-2 which has been amplified by theerbium-doped-fiber 11-1. The thus multiplexed light is introduced intothe erbium-doped-fiber 11-2.

It is to be noted that the erbium-doped-fiber 11-2 at the rear stagereceives pump light from the pump source 12-2 and optical amplifies thesignal light with the pump light.

In particular, in the present first embodiment, the erbium-doped-fiberoptical amplifier of the two stage construction employing the opticalcirculator 15 of the three port type is constructed such that pump light(for example, of 0.98 μm) is introduced into the Input side of the frontstage erbium-doped-fiber 11-1 through the opticaldemultiplexer-multiplexer 13-1 and the optical demultiplexer-multiplexer13-2 is provided on the output side of the front stageerbium-doped-fiber 11-1 such that signal light may be inputted to therear stage erbium-doped-fiber 11-2 through the optical filter 17 and theisolator (ISO) 16-2.

Meanwhile, the pump light is demultiplexed from the signal light by theoptical demultiplexer-multiplexer 13-2 and then reflected by thereflecting mirror 14 so that it goes back through the front stageerbium-doped-fiber 11-1. The pump light is thereafter demultiplexed bythe optical demultiplexer-multiplexer 13-1 and introduced by the opticalcirculator 15 so that it is inputted to the rear stageerbium-doped-fiber 11-2 by way of the optical demultiplexer-multiplexer13-3.

In the optical fiber amplifier shown in FIG. 16, the pump source 12-2 isprovided also on the output side of the rear stage erbium-doped-fiber11-2, and taking possible interference between the pump sources 12-1 and12-2 into consideration, the wavelength of the pump source 12-1 is setto 0.98 μm while the wavelength of the pump source 12-2 is set to 1.47μm so that residual pump light of 0.98 μm is prevented from entering thepump source 12-2 by the optical demultiplexer-multiplexer 13-4.

Thus, in the first embodiment shown in FIG. 16, the optical fiberamplifier wherein the erbium-doped-fibers 11-1 and 11-2 are disposed atthe two front and rear stages includes a first element for introducingpump light into one end of the erbium-doped-fiber 11-1 by way of theoptical circulator 15 and the optical demultiplexer-multiplexer 13-1, asecond element for demultiplexing residual pump light originating fromthe pump light introduced into the one end of the erbium-doped-fiber11-1 by the first element and arriving at the other end of theerbium-doped-fiber 11-1 from signal light using the opticaldemultiplexer-multiplexer 13-2 and then reflecting the residual pumplight using the reflection element 14 so that it is introduced back intothe erbium-doped-fiber 11-1, and a third element for causing theresidual pump light reflected from the reflection element 14 andreturned into the erbium-doped-fiber 11-1 by the reflection element 14to follow a different optical light by means of the optical circulator15 so that it is introduced into and multiplexed by the opticaldemultiplexer-multiplexer 13-3 with the signal light and introducing thethus multiplexed light into the erbium-doped-fiber 11-2.

In the manner, in the present first embodiment, by introducing residualpump power, which is produced when the average pump ratio is set high,back into-the erbium-doped-fiber 11-1 using the opticaldemultiplexer-multiplexer 13-2 and the reflecting mirror 14 providednewly so that the residual pump power may be transmitted backwardlythrough the erbium-doped-fiber 11-1, the pump power can be utilizedefficiently, and consequently, improvement in conversion efficiency canbe achieved.

Further, since the optical circulator 15 is employed in this instance, aloop can be formed to prevent the pump power from becoming unstable.

Furthermore, since a Faraday rotation reflecting mirror is employed forthe reflecting mirror 14, the polarization of pump light can be rotated,and consequently, PHB (Polarization Hole Burning) can be reduced.

B1-1. First Modification to the First Embodiment

FIG. 17 is a block diagram showing a first modification to the firstembodiment of the present invention. Referring to FIG. 17, the modifiedoptical fiber amplifier shown includes an isolator 16-1, an opticaldemultiplexer-multiplexer 13-1, an erbium-doped-fiber 11-1, anotheroptical demultiplexer-multiplexer 13-2, another isolator 16-2, a furtheroptical demultiplexer-multiplexer 13-3, another erbium-doped-fiber 11-2and a further isolator 16-3 disposed in this order from the input side.

A pump source 12-1 is connected to the optical demultiplexer-multiplexer13-1 by way of an optical circulator 15. The optical circulator 15 isconnected, in addition to the pump source 12-1, at another port thereofto the optical demultiplexer-multiplexer 13-3. A reflecting mirror 14.13connected to the optical demultiplexer-multiplexer 13-1.

It can be seen also from the construction described above that, in theoptical fiber amplifier shown in FIG. 17, the erbium-doped-fibers 11-1and 11-2 at the front and rear stages are both pumped by the single pumpsource 12-1. It is to be noted that, while the optical filter 17 isomitted in the arrangement shown in FIG. 17, also the modified opticalfiber amplifier may include the optical filter 17 at the position shownin FIG. 16.

Also in the modified optical fiber amplifier, pump light is introducedinto one end of the erbium-doped-fiber 11-1 from the opticaldemultiplexer-multiplexer 13-1 by way of the optical circulator 15.Then, residual pump light originating from the pump light introducedinto the erbium-doped-fiber 11-1 and arriving at the other end of theerbium-doped-fiber 11-1 is demultiplexed by the opticaldemultiplexer-multiplexer 13-2 and then reflected by the reflectingmirror 14 so that it is introduced back into the erbium-doped-fiber11-1. The reflected residual light introduced into theerbium-doped-fiber 11-1 is introduced, after passing theerbium-doped-fiber 11-1, into a different optical path by the opticalcirculator 15 so that it is introduced into and multiplexed by theoptical demultiplexer-multiplexer 13-3 with signal light, and the thusmultiplexed light is introduced into and amplified by theerbium-doped-fiber 11-2. Consequently, similar advantages or effects tothose of the first embodiment described hereinabove with reference toFIG. 16 can be achieved. In addition, since the pump source 12-1 isprovided commonly for the two erbium-doped-fibers 11-1 and 11-2, theoptical fiber amplifier is simplified in construction and reduced incost.

B1-2. Second Modification to the First Embodiment

FIG. 18 is a block diagram showing a second modification to the firstembodiment of the present invention. Referring to FIG. 18, the modifiedoptical fiber amplifier shown includes an opticaldemultiplexer-multiplexer 13-1, an erbium-doped-fiber 11-1, anotheroptical demultiplexer-multiplexer 13-2, an optical filter 17, anisolator 16-2, a further optical demultiplexer-multiplexer 13-3 andanother erbium-doped-fiber 11-2 disposed in this order from the inputside. Input signal light is inputted by way of an optical circulator15-2 of the four port type, and also output signal light is outputted byway of the same optical circulator 15-2. A pump source 12-1 is connectedto the optical demultiplexer-multiplexer 13-1 by way of another opticalcirculator 15. The optical circulator 15 is connected, in addition tothe pump source 12-1, at another port thereof to the opticaldemultiplexer-multiplexer 13-3. A reflecting mirror 14 is connected tothe optical demultiplexer-multiplexer 13-2.

As can be recognized also from the construction described above, theoptical fiber amplifier shown in FIG. 18 includes the optical circulator15-2 in place of the isolators at the inputting and outputting portionsemployed in the embodiment shown in FIG. 16 and the first modificationshown in FIG. 17.

The optical circulator 15-2 is such an optical circulator of the fourport type as shown in FIGS. 53( a) and 53(b) which is formed from a pairof PBSs, a pair of 45-degree Faraday rotators (non-reciprocal) and apair of 45-degree polarizing rotators (reciprocal) and has ports 1 to 4.

The optical circulator 15-2 outputs an optical signal inputted to theport 1 from the port 2 as seen in FIG. 53( a) but outputs an opticalsignal inputted to the port 2 from the port 3 as seen in FIG. 53( b).Further, though not shown, an optical signal inputted to the port 3 ofthe optical circulator 15-2 is outputted from the port 4, but an opticalsignal inputted to the port 4 is outputted from the port 1 (in thedescription of the embodiments described below, unless otherwisespecified, each optical circulator has the structure shown in FIGS. 53(a) and 53(b)).

The optical circulator 15-2 shown in FIG. 18 is arranged so that aninput optical signal is inputted to the port 1 and an output opticalsignal is outputted from the port 4. The opticaldemultiplexer-multiplexer 13-1 is connected to the port 2 while theerbium-doped-fiber 11-2 is connected to the port 3.

It is to be noted that the optical filter 17 may be omitted.

Also in the present arrangement, pump light is introduced into one endof the erbium-doped-fiber 11-1 from the opticaldemultiplexer-multiplexer 13-1 by way of the optical circulator 15.Then, residual pump light originating from the pump light inputted tothe erbium-doped-fiber 11-1 and arriving at the other end of theerbium-doped-fiber 11-1 is demultiplexed from signal light by theoptical demultiplexer-multiplexer 13-2. The residual pump light isreflected by the reflecting mirror 14 so that it is introduced back intothe erbium-doped-fiber 11-1. Then, the reflected residual pump lightintroduced into the erbium-doped-fiber 11-1 is introduced, after passingthe erbium-doped-fiber 11-1, into a different optical path by theoptical circulator 15 so that it is thereafter multiplexed with thesignal light by the optical demultiplexer-multiplexer 13-3, and the thusmultiplexed light is introduced into and amplified by theerbium-doped-fiber 11-2. Consequently, similar effects to thosedescribed hereinabove in connection with the first embodiment shown inFIG. 16 can be achieved. Further, since the optical circulator 15-2 isprovided at the inputting and outputting portions of the optical fiberamplifier, the number of isolators to be used can be reduced.Consequently, the modified optical fiber amplifier is advantageous alsoin that it can be produced at reduced cost.

B1-3. Third Modification to the First Embodiment

FIG. 19 is a block diagram showing a third modification to the firstembodiment of the present invention. Referring to FIG. 19, the modifiedoptical fiber amplifier shown includes an isolator 16-1, an opticaldemultiplexer-multiplexer (second optical coupler) 13-2′, anerbium-doped-fiber 11-1, an optical demultiplexer-multiplexer (firstoptical coupler) 13-1′, an optical filter 17, another isolator 16-2, afurther optical demultiplexer-multiplexer 13-3, anothererbium-doped-fiber 11-2, a still further opticaldemultiplexer-multiplexer 13-4 and a further isolator 16-3 disposed inthis order from the input side. A pump source 12-1 is connected to theoptical demultiplexer-multiplexer 13-1′ by way of an optical circulator15. The optical circulator 15 is connected, in addition to the pumpsource 12-1, at another port thereof to the opticaldemultiplexer-multiplexer 13-3. A reflecting mirror 14 is connected tothe optical demultiplexer-multiplexer 13-2′. Further, another pumpsource 12-2 is connected to the optical demultiplexer-multiplexer 13-4.

As can be recognized also from the construction described above, in theoptical fiber amplifier shown in FIG. 19, pump light is introduced intothe erbium-doped-fiber 11-1 from the output side of the same. Also inthe present arrangement, the optical filter 17 can be omitted.

In the optical fiber amplifier, pump light is introduced into the outputend of the erbium-doped-fiber 11-1 from the opticaldemultiplexer-multiplexer 13-1′ by way of the optical circulator 15, andresidual pump light originating from the pump light introduced into theerbium-doped-fiber 11-1 and arriving at the input end of theerbium-doped-fiber 11-1 is demultiplexed by the opticaldemultiplexer-multiplexer 13-2′. The residual pump light is thenreflected by the reflecting mirror 14 so that it is introduced back intothe erbium-doped-fiber 11-1. The reflected residual light introducedinto the erbium-doped-fiber 11-1 is introduced, after passing theerbium-doped-fiber 11-1, into a different optical path by the opticalcirculator 15 so that it is thereafter multiplexed with signal light bythe optical demultiplexer-multiplexer 13-3, and the thus multiplexedlight is introduced into and amplified by the erbium-doped-fiber 11-2.

Consequently, similar advantages or effects to those describedhereinabove in connection with the first embodiment of the presentinvention shown in FIG. 16 are achieved.

B1-4. Fourth Modification to the First Embodiment

FIG. 20 is a block diagram showing a fourth modification to the firstembodiment of the present invention. Referring to FIG. 20, the modifiedoptical fiber amplifier shown includes an isolator 16-1, an opticaldemultiplexer-multiplexer 13-2′, an erbium-doped-fiber 11-1, anotheroptical demultiplexer-multiplexer 13-1′, another isolator 16-2, afurther optical demultiplexer-multiplexer 13-3, anothererbium-doped-fiber 11-2, a still further opticaldemultiplexer-multiplexer 13-4, a further isolator 16-3, an opticalfilter 17-2 and a coupler 13-5 disposed in this order from the inputside. Similarly as in the modified optical fiber amplifier shown in FIG.19, a pump source 12-1 is connected to the opticaldemultiplexer-multiplexer 13-1′ by way of an optical circulator 15, andthe optical circulator 15 is connected, in addition to the pump source12-1, at another port thereof to the optical demultiplexer-multiplexer13-3. Further, a reflecting mirror 14 is connected to the opticaldemultiplexer-multiplexer 13-2′. Meanwhile, another pump source 12-2 isconnected to the optical demultiplexer-multiplexer 13-4.

The optical fiber amplifier further includes an output light detector 18for detecting output light from the coupler 13-5, and a constant opticaloutput controller 19 for controlling the pump source 12-2 based on aresult of detection of the output light detector 18 so that the outputof the pump source 12-2 may be constant.

In particular, referring to FIG. 21, the output light detector 18includes a photodiode 18A. A detection value Vin1 by the photodiode 18Ais inputted to a differential amplifier 19A which forms the constantoptical output controller 19. The differential amplifier 19A supplies adifference G1 between a reference value Vref1 and the detection valueVin1 as a control signal Vcont1 to a laser diode which forms the pumpsource 12-2.

The relationship among the output optical power, the control signalVcont1 and the output of the laser diode is such as illustrated in FIG.22.

As can be recognized apparently from the construction described above,the optical fiber amplifier shown in FIG. 20 is so constructed as torealize constant optical output control (ALC).

Also in the present modified optical fiber amplifier, pump light isintroduced into an output end of the erbium-doped-fiber 11-1 from theoptical demultiplexer-multiplexer 13-1′ by way of the optical circulator15 similarly as in the arrangement shown in FIG. 19. Residual pump lightoriginating from the pump light introduced into the erbium-doped-fiber11-1 and arriving at an input end of the erbium-doped-fiber 11-1 isdemultiplexed by the optical demultiplexer-multiplexer 13-2′. Theresidual pump light is reflected by the reflecting mirror 14 so that itis introduced back into the erbium-doped-fiber 11-1. The reflectedresidual light introduced into the erbium-doped-fiber 11-1 isintroduced, after passing the erbium-doped-fiber 11-1, into a differentoptical path by the optical circulator 15 so that it is thereaftermultiplexed with signal light by the optical demultiplexer-multiplexer13-3. The thus multiplexed light is introduced into and amplified by theerbium-doped-fiber 11-2. Then, constant optical output control isapplied to the amplified light under the control of the constant opticaloutput controller 19.

Consequently, similar advantages or effects to those describedhereinabove in connection with the first embodiment of the presentinvention shown in FIG. 16 are achieved. In addition, since constantoptical output control is performed, the optical output level can be setso that it exhibits a reduced accumulation of ASE and a reduceddeterioration in signal to noise ratio (SNR) caused by nonlinear effectsin an optical fiber transmission line.

B1-5. Others

While an erbium-doped-fiber which makes use of reflected residual pumplight is disposed, in the embodiment and its modifications describedabove, at the front stage, the other erbium-doped-fiber provided at therear stage may make use of reflected residual pump light.

B2. Second Embodiment

FIG. 23 is a block diagram showing a second preferred embodiment of thepresent invention. Referring to FIG. 23, the optical fiber amplifiershown includes an isolator 25-1, an optical demultiplexer-multiplexer(first coupler) 24-1, an erbium-doped-fiber (rare earth doped fiber)21-1, another optical demultiplexer-multiplexer (second coupler) 24-2,an optical filter 26, another isolator 25-3, a further opticaldemultiplexer-multiplexer (third coupler) 24-3, anothererbium-doped-fiber (rare earth doped fiber) 21-2, a still furtheroptical demultiplexer-multiplexer (fourth coupler) 24-4 and a furtherisolator 25-4 disposed in this order from the input side.

An optical signal line including the optical filter 26 and the isolator25-3 and a pump light line are provided in parallel between the opticaldemultiplexer-multiplexers 24-2 and 24-3.

A pump source 22 is connected to the optical demultiplexer-multiplexer24-1 by way of an optical branching element 23 and a still furtherisolator 25-2.

The optical branching element 23 branches pump power from the pumpsource 22 (whose wavelength is, for example, 0.98 μm) at the ratio ofn:1 (n is a real number equal to or greater than 1). The light branchedby the optical branching element 23 (and having, for example, lowerpower) is supplied to the optical demultiplexer-multiplexer 24-1 whilethe other light branched by the optical branching element 23 (andhaving, for example, higher power) is supplied to the opticaldemultiplexer-multiplexer 24-4.

In particular, the optical fiber amplifier which includes theerbium-doped-fibers 21-2 and 21-2 disposed at the two front and rearstages as shown in FIG. 23 includes a first element for branching pumppower at the ratio of n:1 (n is a real number equal to or greaterthan 1) by means of the optical branching element 23, multiplexing thepump light from one output port of the optical branching element 23 withsignal light by the optical demultiplexer-multiplexer 24-1 andintroducing the thus multiplexed light into one end of theerbium-doped-fiber 21-1, a second element for extracting residual pumppower originating from the pump light introduced into the one end of theerbium-doped-fiber 21-1 by the first element by means of the opticaldemultiplexer-multiplexer 24-2 connected to the other end of theerbium-doped-fiber 21-1, multiplexing the thus extracted residual pumppower with the signal light by means of the opticaldemultiplexer-multiplexer 24-3 and introducing the thus multiplexedlight into one end of the erbium-doped-fiber 21-2, and a third elementfor multiplexing the pump power from another port of the opticalbranching element 23 branched by the optical branching element 23 withthe light outputted from the other end of the erbium-doped-fiber 21-2 bymeans of the optical demultiplexer-multiplexer 24-4.

In the optical fiber amplifier of the second embodiment having theconstruction described above, pump power is branched at the ratio of n:1(n is a real number equal to or greater than 1) by the optical branchingelement 23, and the pump light from one port of the optical branchingelement 23 is multiplexed with signal light by the opticaldemultiplexer-multiplexer 24-1 and then introduced into theerbium-doped-fiber 21-1 at the front stage.

After the pump light is introduced into the input end of theerbium-doped-fiber 21-1, residual pump power is extracted by the opticaldemultiplexer-multiplexer 24-2 connected to the output end of theerbium-doped-fiber 21-1 and then multiplexed with the signal light bythe optical demultiplexer-multiplexer 24-3. The thus multiplexed lightis introduced into an Input end of the erbium-doped-fiber 21-2 at therear stage. It is to be noted that, while the signal light is inputtedto the erbium-doped-fiber 21-2 at the rear stage by way of the opticalfilter 26 and the isolator 25-3, an ASE portion of the output of theerbium-doped-fiber 21-1 which exhibits a mountain-like shape in outputcharacteristic (for example, a portion at 1.535 μm; refer to FIG. 46) iscut by the optical filter 26 (that is, the mountain is leveled into aflat shape or the shorter wavelength side than 1.538 μm is cut away).

Thereafter, the pump power from the other port of the optical branchingelement 23 branched by the optical branching element 23 is multiplexedwith the signal light outputted from the output end of theerbium-doped-fiber 21-2 by the optical demultiplexer-multiplexer 24-4.

In this manner, in the present second embodiment, residual pump powerwhich is produced when the average pump ratio is raised can be suppliedalso to the other erbium-doped-fiber. Further, since a single pumpsource is used commonly for the two erbium-doped-fibers and thedistribution of the pump power to the erbium-doped-fibers 21-1 and 21-2at the front and rear stages can be set suitably when required, the pumppower can be utilized with a higher degree of efficiency, andconsequently, the conversion efficiency can be improved remarkably.

It is to be noted that the modified optical fiber amplifier may befurther modified such that input signal light is inputted by way of anoptical circulator and output signal light is outputted by way of theoptical circulator in a similar manner as in the arrangement shown inFIG. 18.

B2-1. Modification to the Second Embodiment

FIG. 24 is a block diagram showing a modification to second preferredembodiment of the present invention. Referring to FIG. 24, the modifiedoptical fiber amplifier shown includes an isolator 25-1, an opticaldemultiplexer-multiplexer (second coupler) 24-2′, an erbium-doped-fiber21-1, another optical demultiplexer-multiplexer (first coupler) 24-1′,an optical filter 26, another isolator 25-3, a further opticaldemultiplexer-multiplexer (fourth coupler) 24-4′, anothererbium-doped-fiber 21-2, a still further opticaldemultiplexer-multiplexer (third coupler) 24-3′ and a further isolator25-4 disposed in this order from the input side.

An optical signal line including the optical filter 26 and the isolator25-3 and a pump light line are provided in parallel also between theoptical demultiplexer-multiplexers 24-1′ and 24-4′.

A pump source 22 is connected to the optical demultiplexer-multiplexers24-1′ and 24-4′ by way of an optical branching element 23 and a stillfurther isolator 25-2.

Thus, also the optical fiber amplifier shown in FIG. 24 includes a firstelement for branching pump power at the ratio of n:1 (n is a real numberequal to or greater than 1) by means of the optical branching element23, multiplexing the pump light from one output port of the opticalbranching element 23 with signal light by the opticaldemultiplexer-multiplexer 24-1′ and introducing the thus multiplexedlight into one end of the erbium-doped-fiber 21-1, a second element forextracting residual pump power originating from the pump lightintroduced into the one end of the erbium-doped-fiber 21-1 by the firstelement by means of the optical demultiplexer-multiplexer 24-2′connected to the other end of the erbium-doped-fiber 21-1, multiplexingthe thus extracted residual pump power with the signal light by means ofthe optical demultiplexer-multiplexer 24-3′ and introducing the thusmultiplexed light into one end of the erbium-doped-fiber 21-2, and athird element for multiplexing the pump power from another port of theoptical branching element 23 branched by the optical branching element23 with the light outputted from the other end of the erbium-doped-fiber21-2 by means of the optical demultiplexer-multiplexer 24-4′.

In the modified optical fiber amplifier shown in FIG. 24 and having theconstruction described above, pump power is branched at the ratio of n:1(n is a real number equal to or greater than 1) by the optical branchingelement 23, and pump light from one port of the optical branchingelement 23 is multiplexed with signal light by the opticaldemultiplexer-multiplexer 24-1′ and then introduced into the output endof the erbium-doped-fiber 21-1 at the front stage.

After the pump light is introduced into the output end of theerbium-doped-fiber 21-1, residual pump power is extracted by the opticaldemultiplexer-multiplexer 24-2′ connected to the input end of theerbium-doped-fiber 21-1 and then multiplexed with the signal light bythe optical demultiplexer-multiplexer 24-3′. The thus multiplexed lightis introduced into the output end of the erbium-doped-fiber 21-2 at therear stage. It is to be noted that the signal light is inputted to theerbium-doped-fiber 21-2 at the rear stage by way of the optical filter26 and the isolator 25-3.

Thereafter, the pump power from the other port of the optical branchingelement 23 branched by the optical branching element 23 is multiplexedwith the signal light outputted from the input end of theerbium-doped-fiber 21-2 by the optical demultiplexer-multiplexer 24-4′.

In this manner, also in the modified optical fiber amplifier, residualpump power which is produced when the average pump ratio is raised canbe supplied also to the other erbium-doped-fiber. Further, since asingle pump source is used commonly for the two erbium-doped-fibers andthe distribution of the pump power to the erbium-doped-fibers 21-1 and21-2 at the front and rear stages can be set suitably when required, thepump power can be utilized with a higher degree of efficiency, andconsequently, the conversion efficiency can be improved remarkably.

It is to be noted that also the present modified optical fiber amplifiermay be further modified such that input signal light is inputted by wayof an optical circulator and output signal light is outputted by way ofthe same optical circulator in a similar manner as in the arrangementshown in FIG. 18.

B3. Third Embodiment

FIG. 25 is a block diagram showing a third preferred embodiment of thepresent invention. Referring to FIG. 25, the optical fiber amplifiershown includes an isolator 5-1, an optical demultiplexer-multiplexer3-1, an erbium-doped-fiber (rare earth doped fiber) 1, another opticaldemultiplexer-multiplexer 3-2, and another isolator 5-3 disposed in thisorder from the input side. A pump source 2 is connected to the opticaldemultiplexer-multiplexer 3-1 by way of a further isolator 5-2. Areflecting mirror (reflection element) 4 is connected to the opticaldemultiplexer-multiplexer 3-2.

In particular, the optical fiber amplifier shown in FIG. 25 includes afirst element for introducing pump light into an input end of theerbium-doped-fiber 1 by means of the optical demultiplexer-multiplexer3-1, and a second element for demultiplexing residual pump lightoriginating from the pump light introduced into the input end of theerbium-doped-fiber 1 by the first element and arriving at the output endof the erbium-doped-fiber 1 by means of the opticaldemultiplexer-multiplexer 3-2 and reflecting the residual pump light bymeans of the reflecting element (reflecting mirror) 4 so as to introducethe residual pump light back into the erbium-doped-fiber 1.

A Faraday rotation reflecting mirror is used for the reflecting mirror4.

In the optical fiber amplifier shown in FIG. 25 and having theconstruction described above, pump light is introduced into one end ofthe erbium-doped-fiber 1 by way of the optical demultiplexer-multiplexer3-1, and residual pump light originating from the pump light introducedinto the erbium-doped-fiber 1 and arriving at the other end of theerbium-doped-fiber 1 is demultiplexed by the opticaldemultiplexer-multiplexer 3-2 and then reflected by the reflectingmirror 4 so that it is introduced back into the erbium-doped-fiber 1.

Consequently, also in the present third embodiment, residual pump powerwhich is produced when the average pump ratio is raised is reflectedusing the optical demultiplexer-multiplexer 3-2 and the reflectingmirror 4 prepared newly so as to go back through the erbium-doped-fiber1. Accordingly, the pump power can be utilized efficiently, and as aresult, improvement in conversion efficiency can be achieved.

Further, since a Faraday rotation reflecting mirror is used for thereflecting mirror 4, polarization of pump light can be rotated, andconsequently, the PHB can be reduced.

Also the optical fiber amplifier of the present embodiment may bemodified such that input signal light is inputted by way of an opticalcirculator and output signal light is outputted by way of the sameoptical circulator in a similar manner as in the arrangement shown inFIG. 18.

Further, pump light may alternatively be introduced into the output endof the erbium-doped-fiber 1.

B4. Fourth Embodiment

FIG. 26 is a block diagram showing a fourth preferred embodiment of thepresent invention. Referring to FIG. 26, the optical fiber amplifiershown includes an isolator 5-1, an optical demultiplexer-multiplexer3-1, an erbium-doped-fiber (rare earth doped fiber) 1-1, another opticaldemultiplexer-multiplexer 3-3, another isolator 5-3, a further opticaldemultiplexer-multiplexer 3-4, another erbium-doped-fiber (rare earthdoped fiber) 1-2, a still further optical demultiplexer-multiplexer 3-5,and a further isolator 5-4 disposed in this order from the input side.

An optical signal line including the isolator 5-3 and a pump light lineare provided in parallel between the optical demultiplexer-multiplexers3-3 and 3-4.

Also in the optical fiber amplifier of the present embodiment, a pumpsource 2 is connected to the optical demultiplexer-multiplexer 3-1 byway of a still further isolator 5-2. A reflecting mirror (Faradayrotation reflecting mirror) 4 is connected to the opticaldemultiplexer-multiplexer 3-5.

In the optical fiber amplifier shown in FIG. 26 and having theconstruction described above, pump light is introduced into the inputend of the erbium-doped-fiber 1-1 by the opticaldemultiplexer-multiplexer 3-1. After the pump light is introduced intothe input end of the erbium-doped-fiber 1-1 in this manner, residualpump power is extracted by the optical demultiplexer-multiplexer 3-3connected to the output end of the erbium-doped-fiber 1-1 and thenmultiplexed with signal light by the optical demultiplexer-multiplexer3-4. The thus multiplexed light is introduced into the input end of theerbium-doped-fiber 1-2 at the rear stage. It is to be noted that thesignal light is inputted to the erbium-doped-fiber 1-2 at the rear stageby way of the isolator 5-3.

Thereafter, the residual pump light arriving at the output end of theerbium-doped-fiber 1-2 at the rear stage is demultiplexed by the opticaldemultiplexer-multiplexer 3-5 and then reflected by the reflectingmirror 4 so that it is introduced back into the erbium-doped-fibers 1-2and 1-1.

Consequently, also in the present fourth embodiment, residual pump powerwhich is produced when the average pump ratio is raised is reflectedusing the optical demultiplexer-multiplexer 3-5 and the reflectingmirror 4 prepared newly so as to go back through the erbium-doped-fibers1-2 and 1-1. Accordingly, the pump power can be utilized efficiently,and as a result, improvement in conversion efficiency can be achieved.

Further, since a Faraday rotation reflecting mirror is used for thereflecting mirror 4, polarization of pump light can be rotated, andconsequently, the PHB can be reduced.

Furthermore, also the optical fiber amplifier of the present embodimentmay be modified such that input signal light is inputted by way of anoptical circulator and output signal light is outputted by way of thesame optical circulator in a similar manner as in the arrangement shownin FIG. 18.

While the erbium-doped-fiber which makes use of reflected residual pumplight is provided at a front stage in the embodiment described above,naturally the other erbium-doped-fiber provided at the rear stage maymake use of reflected residual pump light.

B5. Fifth Embodiment

FIG. 27 is a block diagram showing a fifth preferred embodiment of thepresent invention. Referring to FIG. 27, also the optical fiberamplifier shown includes an isolator 39-1, an opticaldemultiplexer-multiplexer 34-1, an erbium-doped-fiber (rare earth dopedfiber) 31, another optical demultiplexer-multiplexer 34-2, and anotherisolator 39-2 disposed in this order from the input side similarly as inthe third embodiment described hereinabove. Further, a pump source 32 isconnected to the optical demultiplexer-multiplexer 34-1 by way of anoptical circulator 33 of the three port type. Furthermore, a reflectingmirror (Faraday rotation reflecting mirror) 35 is connected to theoptical demultiplexer-multiplexer 34-2.

A residual pump light detector 36 is connected to the optical circulator33 so that residual pump light returned into the erbium-doped-fiber 31from the reflecting mirror 35 and inputted to the optical circulator 33by way of the erbium-doped-fiber 31 and the opticaldemultiplexer-multiplexer 34-1 may be detected by the residual pumplight detector 36.

The optical fiber amplifier further includes a controller 37 forcontrolling the pump source 32 so that residual pump light detected bythe residual pump light detector 36 may be constant.

In particular, referring to FIG. 28, the residual pump light detector 36includes a photodiode 36A. A detection value Vin2 by the photodiode 36Ais inputted to a differential amplifier 37A which forms the controller37. The differential amplifier 37A supplies a difference G2 between areference value Vref2 and the detection value Vin2 as a control signalVcont2 to a laser diode which forms the pump source 32.

The relationship among the output optical power, the control signalVcont2 and the output of the laser diode is such as illustrated in FIG.29.

As can be recognized apparently also from the construction describedabove, the optical fiber amplifier shown in FIG. 27 is so constructed asto realize such control of the pump source 32 that residual pump lightdetected by the residual pump light detector 36 may be constant.

Consequently, also with the present fifth embodiment, efficientutilization of the pump power can be achieved and improvement inconversion efficiency can be achieved. In addition, by monitoring theresidual pump power, the average pump ratio can be kept constant to keepthe wavelength dependency of the gain constant with respect to thevariation of the input power.

B5-1. First Modification to the Fifth Embodiment

FIG. 30 is a block diagram showing a first modification to the fifthembodiment of the present invention. The modified optical fiberamplifier shown in FIG. 30 is a modification to the optical fiberamplifier of the construction shown in FIG. 27 in that Input signallight is inputted by way of an optical circulator 38, which is providedadditionally, and output signal light is outputted by way of the sameoptical circulator 38. Due to the construction, advantages or effectsachieved by the fifth embodiment described above can be achieved, andbesides, since the optical circulator 38 is provided at the input andoutput portions of the optical fiber amplifier, the modified opticalfiber amplifier is advantageous in that the number of isolators to beused can be reduced and reduction in cost can be achieved.

B5-2. Second Modification to the Fifth Embodiment

FIG. 31 is a block diagram showing a second modification to the fifthembodiment of the present invention. The modified optical fiberamplifier shown in FIG. 31 includes an isolator 39-1, an opticaldemultiplexer-multiplexer 34-2′, an erbium-doped-fiber 31-1, anotheroptical demultiplexer-multiplexer 34-1′, an optical filter 40, anotherisolator 39-3, a further optical demultiplexer-multiplexer 34-1″,another erbium-doped-fiber 31-2, a still further opticaldemultiplexer-multiplexer 34-2″, and a further isolator 39-2 disposed inthis order from the input side.

A pump source 32 is connected to the optical demultiplexer-multiplexers34-1′ and 34-1″ by way of an optical circulator 33′ of the four porttype. Furthermore, a pair of reflecting mirrors (Faraday rotationreflecting mirrors) 35′ and 35″ are connected to the opticaldemultiplexer-multiplexers 34-2′ and 34-2″, respectively.

A residual pump light detector 36 is connected to the optical circulator33′ so that residual pump light returned into the erbium-doped-fibers31-1 and 31-2 from the reflecting mirrors 35′ and 35″ and inputted tothe optical circulator 33′ by way of the erbium-doped-fibers 31-1 and31-2 and the optical demultiplexer-multiplexers 34-1′ and 34-1″,respectively, may be detected by the residual pump light detector 36.

The optical fiber amplifier further includes a controller 37 forcontrolling the pump source 32 so that residual pump light detected bythe residual pump light detector 36 may be constant.

As can be recognized apparently also from the construction describedabove, the optical fiber amplifier shown in FIG. 31 is so constructed asto realize such control of the pump source 32 that residual pump lightfrom the erbium-doped-fibers 31-1 and 31-2 detected by the residual pumplight detector 36 may be constant.

Consequently, also with the modified optical fiber amplifier, similaradvantages or effects to those of the fifth embodiment described abovecan be achieved.

Furthermore, also the modified optical fiber amplifier may be modifiedsuch that input signal light is inputted by way of an optical circulatorand output signal light is outputted by way of the same opticalcirculator in a similar manner as in the arrangement shown in FIG. 30.

B6. Sixth Embodiment

FIG. 32 is a block diagram showing a sixth preferred embodiment of thepresent invention. The optical fiber amplifier shown in FIG. 32 includesan isolator 144, a dispersion compensating fiber 141 and a opticaldemultiplexer-multiplexer 143 disposed in this order from the inputside. A pump source 142 is connected to the opticaldemultiplexer-multiplexer 143.

The pump source 142 is formed from a pump source which produces pumplight of a band (for example, from 1.44 to 1.49 μm) in which bandcompensation for erbium-doped-fiber amplification by Raman amplificationcan be performed pump light from the pump source 142 is introduced intoan output end of the dispersion compensating fiber 141 by way of theoptical demultiplexer-multiplexer 143.

Accordingly, the optical fiber amplifier includes a dispersioncompensating fiber module which includes the dispersion compensatingfiber 141 and the pump source 142.

Due to the construction described above, the dispersion compensatingfiber 141 can be pumped with pump light from the pump source 142 tocause Raman amplification to occur. In particular, since the mode fielddiameter of the dispersion compensating fiber 141 is generally small,the threshold level of the Raman amplification is low, and consequently,Raman amplification occurs readily.

By the way, the dispersion compensating fiber has the followingcharacteristic.

In particular, the dispersion compensating fiber (DCF) is so small indiameter that the mode field diameter thereof is approximately one halfthat of an ordinary fiber and provides nonlinear effects (stimulatedRaman scattering (SRS), stimulated Brillouin scattering (SBS), four wavemixing (FWM), self phase modulation effect (SPM) and so forth) morelikely than a fiber which is used as a transmission line. It is to benoted that, since the dispersion compensating fiber is, in its form ofuse, not so long as a fiber which is used as a transmission line, it isknown that it can be used if the optical power of light to pass it isset low. This is because also the influence of nonlinear effectsincreases as the length increases.

Also it is known that the the attenuation (loss) of light by thedispersion compensating fiber is not ignorable, and accordingly, theloss must be compensated for using an optical amplifier.

Meanwhile, the input power is restricted to a low value as describedhereinabove, which makes it difficult to design the level as an opticalamplifier.

However, some of the nonlinear effects mentioned above are harmful uponcommunication, but some others are useful for communication. Among thenonlinear effects, the Raman amplification is useful.

The Raman amplification may possibly be very useful in the followingpoint. In particular, if a dispersion compensating fiber performs Ramanamplification, then the dispersion compensating fiber itself acts as anoptical amplifier and can compensate for the loss.

It is to be noted that the Raman amplification signifies that, makinguse of stimulated Raman scattering, that is, a phenomenon that, whenintense monochromatic light is irradiated upon an optical fiber, itcoacts with optical phonons of the optical fiber so that coherent Stokeslight displaced by an intrinsic amount in wavelength is generated bystimulated emission, the wavelength of the monochromatic light is set sothat the Stokes light may have an equal wavelength to that of the signallight thereby to amplify the signal light by stimulated emission.

Accordingly, by pumping the dispersion compensating fiber 141 with pumplight of the band described above from the pump source 142 to causeRaman amplification to occur as described above, compensation for theloss of the dispersion compensating fiber (Including leveling of aconcave in gain of an erbium-doped fiber and complementary compensationfor a decrease in gain of an erbium-doped-fiber) can be achieved by theRaman amplification.

It is to be noted that, in order to level a concave in gain in the 1.54μm band of an erbium-doped-fiber, the erbium-doped-fiber is pumped withpump light of the wavelength equal to or less than 1.44 μm to causeRaman amplification to occur.

It is to be noted that another isolator 144-2 may be additionallyprovided on the output side as seen in FIG. 33.

The optical fiber amplifier of the present embodiment may be modifiedotherwise such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions of the opticalfiber amplifier as seen in FIGS. 32 or 33, input signal light isinputted by way of an optical circulator and output signal light isoutputted by way of the same optical circulator in a similar manner asin the arrangement shown in FIGS. 18 or 30.

Further, a silica-type-optical-fiber may be employed in place of thedispersion compensating fiber 141.

B7. Seventh Embodiment

FIG. 34 is a block diagram showing a seventh preferred embodiment of thepresent invention. Referring to FIG. 34, the optical fiber amplifiershown includes an isolator 55-1, an optical demultiplexer-multiplexer54-1, an erbium-doped-fiber (rare earth doped fiber) 51, anotherisolator 55-2, a dispersion compensating fiber 52, another opticaldemultiplexer-multiplexer 54-2 and a further isolator 55-3 disposed inthis order from the input side. Further, a pump source 53-1 is connectedto the optical demultiplexer-multiplexer 54-1 while another pump source53-2 is connected to the optical demultiplexer-multiplexer 54-2.

The pump source 53-1 produces pump light of a first wavelength band forthe erbium-doped-fiber 51 (for example, the 0.98 μm band), and the pumpsource 53-2 produces pump light of a second wavelength band for thedispersion compensating fiber 52 (for example, the 1.47 μm band (1.45 to1.49 μm) or the band up to 1.44 μm (equal to or less than 1.44 μm).

Consequently, the dispersion compensating fiber 52 can be pumped withpump light from the pump source 53-2 to cause Raman amplification tooccur in accordance with the same principle as that of the sixthembodiment described hereinabove. Accordingly, also in the presentembodiment, by pumping the dispersion compensating fiber 52 with pumplight of the 1.47 μm band or the band up to 1.44 μm from the pump source53-2 to cause Raman amplification to occur, compensation for the loss ofthe dispersion compensating fiber can be achieved by the Ramanamplification.

Further, while the wavelength characteristic of the gain of a rare earthdoped fiber optical amplifier depends upon rare earth ions, thewavelength characteristic of the gain of a Raman optical amplifierdepends upon the pump wavelength and the peak value thereof is shiftedif the pump wavelength is changed. Accordingly, the pump wavelength whenRaman amplification is performed can be selected so that the wavelengthcharacteristic of the gain of the rare earth doped fiber opticalamplifier may be compensated for. This allows realization of an opticalamplifier of a wide bandwidth.

In particular, also the Raman amplification involves an amplificationband, and if the wavelength dependency of the gain by the Ramanamplification is utilized, not only mere compensation for the loss of adispersion compensating fiber can be achieved, but also theamplification bandwidth of an erbium-doped-fiber can be complemented toincrease the bandwidth.

In other words, since the wavelength characteristic of anerbium-doped-fiber amplifier is not flat as seen in FIGS. 46 or 47, bycausing Raman amplification to occur using a dispersion compensatingfiber, the unevenness of the wavelength characteristic of theerbium-doped-fiber amplifier can be leveled. As a result, a widebandwidth optical amplifier can be realized, which is suitably used formultiple wavelength collective amplification (refer to FIG. 47) or thelike.

It is to be noted that the rare earth doped fiber optical amplificationelement formed from an erbium-doped-fiber which is a rare earth dopedfiber may be constructed as an optical amplification element having alow noise index.

Further, while the optical fiber amplifier shown in FIG. 34 isconstructed such that the rare earth doped fiber optical amplificationelement formed from an erbium-doped-fiber is disposed as a front stageamplification element while the Raman optical amplification elementformed from a dispersion compensating fiber is disposed as a rear stageamplification element, the construction of the optical fiber amplifieris not limited to the specific one described above and may beconstructed otherwise such that a Raman optical amplification elementformed from a dispersion compensating fiber or asilica-type-optical-fiber is disposed as a front stage amplificationelement while a rare earth doped fiber optical amplification elementformed from an erbium-doped-fiber is disposed as a rear stageamplification element (where such Raman optical amplification element isformed from a silica-type-optical-fiber, a single pump source can beused commonly as a pump source for the silica-type-optical-fiber andanother pump source for the erbium-doped-fiber).

Further, the pump source 53-2 may be formed, for example, from a pair ofpump sources and a polarizing multiplexer for orthogonally polarizingand multiplexing pump light from the pump sources similarly to pumpsources 53-2, 53-2′ and 53-2″ shown in FIGS. 43 to 45. Or the pumpsource 53-2 may otherwise be formed from a combination of a pump sourceand a depolarizer by which pump light is depolarized or else may beformed so as to generate modulated pump light.

It is to be noted that the pump sources 53-2, 53-2′ and 53-2″ shown inFIGS. 43 to 45 will be hereinafter described in connection with afourteenth embodiment of the present invention and first and secondmodifications to the fourteenth embodiment, respectively.

B8. Eighth Embodiment

FIG. 35 is a block diagram showing an eighth preferred embodiment of thepresent invention. Referring to FIG. 35, the optical fiber amplifiershown includes an isolator 65-1, an optical demultiplexer-multiplexer64, an erbium-doped-fiber (rare earth doped fiber) 61, another isolator65-2, a dispersion compensating fiber 62, and a further isolator 65-3disposed in this order from the input side. A pump source 63 isconnected to the optical demultiplexer-multiplexer 64.

The pump source 63 produces pump light, for example, of the 1.47 μm band(1.45 to 1.49 μm).

In the optical fiber amplifier shown in FIG. 35 and having theconstruction described above, pump light is introduced into one end ofthe erbium-doped-fiber 61 from the optical demultiplexer-multiplexer 64to pump the erbium-doped-fiber 61 to amplify signal light. Consequently,residual pump light arrives at the other end of the erbium-doped-fiber61. Thereafter, the residual pump light is supplied by way of theisolator 65-2 to the dispersion compensating fiber 62 so that Ramanamplification may occur in the dispersion compensating fiber 62.

The reason why signal light can be amplified by both of theerbium-doped-fiber and the dispersion compensating fiber using thecommon pump source to them is such as follows.

In particular, the pump wavelength band when signal light of the 1.55 μmband is Raman amplified is the 1.47 μm band (1.45 to 1.49 μm) which isthe pump wavelength band of the erbium-doped-fiber (EDF), andaccordingly, Raman amplification can be caused to occur using residualpump power when the EDF is pumped with light of the 1.47 band. From thisreason, while optical amplification is performed by theerbium-doped-fiber 61, the loss of the dispersion compensating fiber 62can be compensated for.

Consequently, similarly as in the seventh embodiment describedhereinabove, a wide bandwidth optical amplifier wherein the unevennessof the wavelength characteristic of the erbium-doped-fiber amplifier isleveled can be realized, and the wide bandwidth optical amplifier can besuitably applied to multiple wavelength collective amplification.Further, since the single pump source is involved, the optical fiberamplifier can be constructed in simplified structure and at a reducedcost.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions of the opticalfiber amplifier, input signal light is inputted by way of an opticalcirculator and output signal light is outputted by way of the opticalcirculator in a similar manner as in the arrangement shown in FIGS. 18or 30.

Further, the pump source 63 may alternatively be formed from two pumpsources and a polarizing multiplexer which orthogonally polarizes andmultiplexes pump light from the pump sources or may otherwise be formedfrom a combination of a pump source and a depolarizer by means of whichpump light is depolarized or else may generate modulated pump light.

B8-1. First Modification to the Eighth Embodiment

FIG. 36 is a block diagram showing a first modification to the eighthembodiment of the present invention. Referring to FIG. 36, the opticalfiber amplifier shown includes an isolator 65-1, an opticaldemultiplexer-multiplexer 64-1, an erbium-doped-fiber (rare earth dopedfiber) 61-1, another isolator 65-2, a dispersion compensating fiber 62,another erbium-doped-fiber (rare earth doped fiber) 61-2, anotheroptical demultiplexer-multiplexer 64-2 and a further isolator 65-3disposed in this order from the input side. A pump source 63-1 isconnected to the optical demultiplexer-multiplexer 64-1, and anotherpump source 63-2 is connected to the optical demultiplexer-multiplexer64-2.

The pump source 63-1 and 63-2 both produce pump light of, for example,the 1.47 μm band (1.45 to 1.49 μm).

In the optical fiber amplifier shown in FIG. 36 and having theconstruction described above, pump light from the pump source 63-1 isintroduced into an input end of the erbium-doped-fiber 61-1 from theoptical demultiplexer-multiplexer 64-1 to pump the erbium-doped-fiber61-1 to amplify signal light. Consequently residual pump light arrivesat the other end of the erbium-doped-fiber 61-1. Thereafter, theresidual pump light is supplied by way of the isolator 65-2 to thedispersion compensating fiber 62 so that Raman amplification may occurin the dispersion compensating fiber 62.

Meanwhile, pump light from the pump source 63-2 is introduced into anoutput end of the erbium-doped-fiber 61-2 by way of the opticaldemultiplexer-multiplexer 64-2 to pump the erbium-doped-fiber 61-2 toamplify the signal light. Also in this instance, residual pump lightarrives at an input end of the erbium-doped-fiber 61-2. Further, alsothe residual pump light is supplied to the dispersion compensating fiber62 so that Raman amplification may occur in the dispersion compensatingfiber 62.

In this instance, since the dispersion compensating fiber 62 causesRaman amplification to occur using the residual pump light from theerbium-doped-fibers 61-1 and 61-2 on the front and rear sides, thedispersion compensating fiber 62 exhibits a higher compensation effectas much. Consequently, a wide bandwidth optical amplifier can berealized while achieving simplification in structure and reduction incost.

Also the present modified optical fiber amplifier may be furthermodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, a pump source and an optical demultiplexer-multiplexer for thedispersion compensating fiber 62 may be provided additionally.

In particular, similarly as in the optical fiber amplifier of FIG. 12,an optical fiber amplifier may be constructed using pump sources 133-1to 133-3 of the 0.98 μm band and optical demultiplexer-multiplexers134-1 to 134-3.

Furthermore, a silica-type-optical-fiber may be employed in place of thedispersion compensating fiber 62.

B8-2. Second Modification to the Eighth Embodiment

FIG. 37 is a block diagram showing a second modification to the eighthembodiment of the present invention. Referring to FIG. 37, the opticalfiber amplifier shown includes an isolator 65-1, an opticaldemultiplexer-multiplexer 64-1, an erbium-doped-fiber 61-1, anotherisolator 65-2, a dispersion compensating fiber 62, another opticaldemultiplexer-multiplexer 64-3, an optical filter 66, a further isolator65-3, a further optical demultiplexer-multiplexer 64-4, anothererbium-doped-fiber 61-2, a still further opticaldemultiplexer-multiplexer 64-5, and a still further isolator 65-4disposed in this order from the input side. A pump source 63-1 isconnected to the optical demultiplexer-multiplexer 64-1, and anotherpump source 63-2 is connected to the optical demultiplexer-multiplexer64-5.

The pump sources 63-1 and 63-2 both produce pump light, for example, ofthe 1.47 μm band (1.45 to 1.49 μm).

An optical signal line including the optical filter 66 and the isolator65-3 and a pump light line are disposed in parallel between the opticaldemultiplexer-multiplexers 64-3 and 64-4.

In the optical fiber amplifier shown in FIG. 37 and having theconstruction described above, pump light from the pump source 63-1 isintroduced into an input end of the erbium-doped-fiber 61-1 by way ofthe optical demultiplexer-multiplexer 64-1 to pump theerbium-doped-fiber 61-1 to amplify signal light. Thereupon, residualpump light arrives at the other end of the erbium-doped-fiber 61-1. Theresidual pump light is supplied to the dispersion compensating fiber 62by way of the isolator 65-2 to cause Raman amplification to occur.

Simultaneously, pump light from the pump source 63-2 is introduced intoan output end of the erbium-doped-fiber 61-2 by way of the opticaldemultiplexer-multiplexer 64-5 to pump the erbium-doped-fiber 61-2 toamplify the signal light. In this instance, residual pump light arrivesat the input end of the erbium-doped-fiber 61-2. Also the residual pumplight is supplied by way of the optical demultiplexer-multiplexers 64-4and 64-3 to the dispersion compensating fiber 62 to cause Ramanamplification to occur.

Also in the present modified optical fiber amplifier, since thedispersion compensating fiber 62 causes Raman amplification to occurusing the residual pump light from the erbium-doped-fibers 61-1 and 61-2at the front and the rear to the dispersion compensating fiber 62, thedispersion compensating fiber 62 exhibits a higher compensation effectas much. Thus, a wide bandwidth optical amplifier can be realized whileachieving simplification in structure and reduction in cost.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Further, a pump source and an optical demultiplexer-multiplexer for thedispersion compensating fiber 62 may be provided additionally.

In particular, similarly as in the optical fiber amplifier of FIG. 12,an optical fiber amplifier may be constructed using pump sources 133-1to 133-3 of the 0.98 μm band and optical demultiplexer-multiplexers134-1 to 134-3.

Furthermore, a silica-type-optical-fiber may be employed in place of thedispersion compensating fiber 62.

B9. Ninth Embodiment

FIG. 38 is a block diagram showing a ninth preferred embodiment of thepresent invention. Referring to FIG. 38, the optical fiber amplifiershown includes an isolator 75-1, an erbium-doped-fiber (rare earth dopedfiber) 71, a dispersion compensating fiber 72, an opticaldemultiplexer-multiplexer 74, and another isolator 75-2 disposed in thisorder from the input side. A pump source 73 is connected to the opticaldemultiplexer-multiplexer 74.

The pump source 73 produces pump light, for example, of the 1.47 μm band(1.45 to 1.49 μm).

In the optical fiber amplifier shown in FIG. 38 and having theconstruction described above, pump light is introduced into an outputside of the dispersion compensating fiber 72 by way of the opticaldemultiplexer-multiplexer 74 to cause Raman amplification to occur.Then, residual pump light from the dispersion compensating fiber 72 isintroduced into an output end of the erbium-doped-fiber 71 to pump theerbium-doped-fiber 71 to amplify signal light.

By pumping the erbium-doped-fiber 71 reversely with residual pump lightupon Raman amplification in this manner, the unevenness of thewavelength characteristic of the erbium-doped-fiber can be leveled torealize a wide bandwidth optical amplifier similarly as in the seventhembodiment described above. The wide bandwidth optical amplifier can beapplied suitably to multiple wavelength collective amplification.Further, since the only single pump source is required, the opticalfiber amplifier of the present embodiment is simplified in structure andreduced in cost.

The reason why the erbium-doped-fiber and the dispersion compensatingfiber can amplify signal light using the pump source common to them isthe same as described above.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Meanwhile, the pump source 73 may be formed from a pair of pump sources,and a polarizing multiplexer for orthogonally polarizing andmultiplexing pump light from the pump sources or may be formed from acombination of a pump source and a depolarizer by which pump light isdepolarized or else may generate modulated pump light.

B10. Tenth Embodiment

FIG. 39 is a block diagram showing a tenth preferred embodiment of thepresent invention. Referring to FIG. 39, the optical fiber amplifiershown includes an isolator 84-1, an optical demultiplexer-multiplexer83, a dispersion compensating fiber 81 (hereinafter referred to aserbium doped dispersion compensating fiber) doped with erbium (rareearth element) ions, and another isolator 84-2 disposed in this orderfrom the input side. A pump source 82 which produces pump light of, forexample, the 1.47 μm band (1.45 to 1.49 μm) or 0.98 μm is connected tothe optical demultiplexer-multiplexer 83.

In the optical fiber amplifier shown in FIG. 39 and having theconstruction described above, pump light is introduced into one end ofthe erbium doped dispersion compensating fiber 81 by way of the opticaldemultiplexer-multiplexer 83 to pump the erbium doped dispersioncompensating fiber 81 to amplify signal light.

Where the core of the dispersion compensating fiber is doped with Erions in this manner, the pump light is attenuated rapidly in the erbiumdoped dispersion compensating fiber 81, and consequently, Ramanamplification does not occur and the loss of the erbium doped dispersioncompensating fiber 81 is compensated for in individual small sections.Consequently, a good signal to noise ratio can be maintained.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, the pump source 82 may be formed from a pair of pump sources,and a polarizing multiplexer for orthogonally polarizing andmultiplexing pump light from the pump sources or may be formed from acombination of a pump source and a depolarizer by which pump light isdepolarized or else may generate modulated pump light.

B11. Eleventh Embodiment

FIG. 40 is a block diagram showing an eleventh preferred embodiment ofthe present invention. Referring to FIG. 40, the optical fiber amplifiershown includes an isolator 96-1, an optical demultiplexer-multiplexer94, an erbium-doped-fiber (rear earth doped fiber) 91, another isolator96-2, an optical filter 95, and a dispersion compensating fiber 92disposed in this order from the input side. A pump source 93 whichproduces pump light of, for example, the 1.47 μm band (1.45 to 1.49 μm)is connected to the optical demultiplexer-multiplexer 94.

The optical filter 95 intercepts residual pump light of the 1.47 μm bandcoming out from the erbium-doped-fiber 91.

In the optical fiber amplifier shown in FIG. 40 and having theconstruction described above, pump light is introduced into one end ofthe erbium-doped-fiber 91 by way of the opticaldemultiplexer-multiplexer 94 to pump the erbium-doped-fiber 91 toamplify signal light. Thereupon, residual pump light arrives at theother end of the erbium-doped-fiber 91. Then, the residual pump light isintercepted by the optical filter 95.

If light of the 1.47 μm band is unnecessarily transmitted through thedispersion compensating fiber 92, then it will disturb the wavelengthcharacteristic of the level diagram designing or the optical amplifierdue to Raman amplification. Therefore, in this instance, light of the1.47 μm band is intercepted by the optical filter 95 so that it may beprevented from being inputted to the dispersion compensating fiber 92.

Accordingly, the dispersion compensating fiber 92 is used to principallycompensate for the dispersion of the transmission line.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is Inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, the pump source 93 may be formed from a pair of pump sources,and a polarizing multiplexer for orthogonally polarizing andmultiplexing pump light from the pump sources or may be formed from acombination of a pump source and a depolarizer by which pump light isdepolarized or else may generate modulated pump light.

B12. Twelfth Embodiment

FIG. 41 is a block diagram showing a twelfth preferred embodiment of thepresent invention. Referring to FIG. 41, the optical fiber amplifiershown includes an isolator 5-1, an optical demultiplexer-multiplexer3-1, an erbium-doped-fiber (rare earth doped fiber) 1 containing silicaas a host component, another optical demultiplexer-multiplexer 3-2, andanother isolator 5-2 disposed in this order from the input side. A pumpsource 2-1 for producing pump light of, for example, the 0.98 μm band isconnected to the optical demultiplexer-multiplexer 3-1. Meanwhile,another pump source 2-2 which produces pump light of, for example,approximately 1.44 μm or approximately 1.46 μm is connected to theoptical demultiplexer-multiplexer 3-2.

Here, the reason why an optical demultiplexer-multiplexer not of thebulk type but of the fusion type is used for the opticaldemultiplexer-multiplexer 3-1 and a pump source of the type which doesnot have a built-in optical isolator (optical ISO) is used for the pumpsource 2-1 is that noise light of the 1.55 μm band which is produced inthe erbium-doped-fiber 1 when an optical signal of the 1.55 μm band isamplified does not return into the pump source 2-1 by which pump lightof the 0.98 μm band is produced (this similarly applies to theembodiments hereinafter described).

In the optical fiber amplifier shown in FIG. 41 and having theconstruction described above, pump light of the 0.98 am band isintroduced into one end of the erbium-doped-fiber 1 by way of theoptical demultiplexer-multiplexer 3-1 to pump the erbium-doped-fiber 1to amplify signal light. Further, pump light of 1.44 μm or pump light of1.46 μm is introduced into an output end of the erbium-doped-fiber 1 byway of the optical demultiplexer-multiplexer 3-2 to cause Ramanamplification to occur in the erbium-doped-fiber 1.

It is known that Raman amplification occurs with an erbium-doped-fibersuch as the erbium-doped-fiber 1 when intense light is inputted to it.

By amplifying signal light with an ordinary pump wavelength (forexample, 0.98 μm (or alternatively 1.47 μm)) using theerbium-doped-fiber 1 which contains silica as a host component and Ramanamplifying the signal light with the wavelength equal to or less than1.44 μm, a concave (refer to FIG. 46) of the gain of the 1.54 μm band ofthe erbium-doped-fiber can be leveled. Further, by Raman amplifying thesignal light with the wavelength of equal to or less than 1.46 μm, thedecrease in gain (refer to FIG. 46) of the erbium-doped-fiber in theproximity of 1.57 μm can be compensated for to level the characteristicthereby to realize an optical fiber amplifier of a wide bandwidth.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

B13. Thirteenth Embodiment

FIG. 42 is a block diagram showing a thirteenth preferred embodiment ofthe present invention. Referring to FIG. 42, the optical fiber amplifiershown includes an isolator 144-1, a dispersion compensating fiber 141, apolarization keeping optical demultiplexer-multiplexer 143 and anotherisolator 144-2 disposed in this order from the input side. Apolarization keeping pump source 142 is connected to the opticaldemultiplexer-multiplexer 143.

The pump source 142 is formed from a pair of pump sources 142A and 142B,and a polarizing multiplexer. (PBS) 142C for orthogonally polarizing andmultiplexing pump light from the pump sources 142A and 142B.

The pump sources 142A and 142B have an equal pump power and output pumplight of, for example, 1.45 to 1.49 μm (or 1.45 to 1.48 μm).

It is to be noted that an optical demultiplexer-multiplexer of theoptical film type is used for the optical demultiplexer-multiplexer 143so that multiplexing or demultiplexing of light may be performed whilemaintaining polarization conditions of the light.

In the optical fiber amplifier shown in FIG. 42 and having theconstruction described above, orthogonally polarized multiplexed pumplight is introduced into an output end of the dispersion compensatingfiber 141 by way of the optical demultiplexer-multiplexer 143 so thatRaman amplification may occur effectively in the dispersion compensatingfiber 141. Thus, the loss of the dispersion compensating fiber can becompensated for by such Raman amplification.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, the dispersion compensating fiber 141 may be replaced by asilica-type-optical-fiber.

Furthermore, the pump source 142 may be constructed, for example, from acombination of a pump source and a depolarizer so that pump light may bedepolarized similarly to the pump source 53-2′ or 53-2″ shown in FIGS.44 or 45 or may generate modulated pump light.

It is to be noted that the pump sources 53-2′ and 53-2″ shown in FIGS.44 and 45 will be described below in connection with first and secondmodifications to a fourteenth embodiment of the present embodiment.

B14. Fourteenth Embodiment

FIG. 43 is a block diagram showing a fourteenth preferred embodiment ofthe present invention. Referring to FIG. 43, the optical fiber amplifiershown includes an isolator 55-1, an optical demultiplexer-multiplexer54-1, an erbium-doped-fiber (rare earth doped fiber) 51, anotherisolator 55-2, a dispersion compensating fiber 52, a polarizationkeeping optical demultiplexer-multiplexer 54-2 and a further isolator55-3 disposed in this order from the input side. Further, a pump source53-1 is connected to the optical demultiplexer-multiplexer 54-1 while apump source 53-2 of the polarization multiplexing type is connected tothe optical demultiplexer-multiplexer 54-2.

The pump source 53-1 outputs pump light of, for example, the 0.98 μmband. Meanwhile, the pump source 53-2 is formed from a pair of pumpsources 53-2A and 53-2B, and a polarizing multiplexer (PBS) 53-2C fororthogonally polarizing and multiplexing pump light from the pumpsources 53-2A and 53-2B.

Also in this instance, the pump sources 53-2A and 53-2B have an equalpump power and both output pump light of, for example, 1.45 to 1.49 μm(or 1.45 to 1.48 μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 54-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 54-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 43 and having theconstruction described above, pump light from the pump source 53-1 isinputted to one end of the erbium-doped-fiber 51 from the opticaldemultiplexer-multiplexer 54-1 together with signal light. Consequently,the signal light is amplified in the erbium-doped-fiber 51.

Meanwhile, orthogonally polarized multiplexed pump light is introducedinto an output end of the dispersion compensating fiber 52 by way of theoptical demultiplexer-multiplexer 54-2 to cause Raman amplification tooccur effectively in the dispersion compensating fiber 52. Thus, theloss of the dispersion compensating fiber 52 is compensated for by suchRaman amplification.

Similar advantages or effects to those of the thirteenth embodimentdescribed above can be achieved also by the optical fiber amplifier ofthe present embodiment.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, the rare earth doped fiber optical amplification element formedfrom an erbium-doped-fiber may be formed as an optical amplificationelement which has a low noise figure. Or, a Raman optical amplificationelement formed from a dispersion compensating fiber may be disposed as afront stage amplification element while a rare earth doped fiber opticalamplification element formed from an erbium-doped-fiber is disposed as arear stage amplification element.

B14-1. First Modification to the Fourteenth Embodiment

FIG. 44 is a block diagram showing a first modification to thefourteenth embodiment of the present invention. Referring to FIG. 44,the optical fiber amplifier shown includes an isolator 55-1, an opticaldemultiplexer-multiplexer 54-1, an erbium-doped-fiber (rare earth dopedfiber) 51, another isolator 55-2, a dispersion compensating fiber 52, apolarization keeping optical demultiplexer-multiplexer 54-2 and afurther isolator 55-3 disposed in this order from the input side.Further, a pump source 53-1 is connected to the opticaldemultiplexer-multiplexer 54-1 while a pump source 53-2′ of thedepolarization multiplexing type is connected to the opticaldemultiplexer-multiplexer 54-2.

The pump source 53-1 produces pump light of, for example, 0.98 μm.Meanwhile, the pump source 53-2′ is formed from a single pump source53-2A′, and a depolarizer 53-2B′ for depolarizing pump light from thepump source 53-2A′.

The depolarizer 53-2B′ reduces the polarization dependency of the Ramanoptical amplifier formed from the dispersion compensating fiber 52 andis formed from a polarization keeping coupler 53-2E′ for demultiplexingpump light from the pump source 53-2A′, and a polarizing multiplexer(PBS) 53-2C′ for orthogonally polarizing and multiplexing pump lightdemultiplexed by the polarization keeping coupler 53-2E′ and pump lightdelayed by a delay line.

Also in the modified optical fiber amplifier, the pump source 53-2A′outputs pump light of, for example, 1.45 to 1.49 μm (or 1.45 to 1.48μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 54-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 54-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 44 and having theconstruction described above, pump light from the pump source 53-1 isinputted to one end of the erbium-doped-fiber 51 from the opticaldemultiplexer-multiplexer 54-1 together with signal light. Consequently,the signal light is amplified in the erbium-doped-fiber 51.

Meanwhile, depolarized pump light is introduced into an output end ofthe dispersion compensating fiber 52 by way of the opticaldemultiplexer-multiplexer 54-2 to cause Raman amplification to occureffectively in the dispersion compensating fiber 52. Thus, the loss ofthe dispersion compensating fiber 52 is compensated for by such Ramanamplification.

By the construction described above, similar advantages or effects tothose of the fourteenth embodiment described above can be achieved whiledecreasing the polarization dependency of the dispersion compensatingfiber 52.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Further, the rare earth doped fiber optical amplification element formedfrom an erbium-doped-fiber may be formed as an optical amplificationelement which has a low noise figure. Or, a Raman optical amplificationelement formed from a dispersion compensating fiber may be disposed as afront stage amplification element while a rare earth doped fiber opticalamplification element formed from an erbium-doped-fiber is disposed as arear stage amplification element.

B14-2. Second Modification to the Fourteenth Embodiment

FIG. 45 is a block diagram showing a second modification to thefourteenth embodiment of the present invention. Referring to FIG. 45,the optical fiber amplifier shown includes an isolator 55-1, an opticaldemultiplexer-multiplexer 54-1, an erbium-doped-fiber (rare earth dopedfiber) 51, another isolator 55-2, a dispersion compensating fiber 52, apolarization keeping optical demultiplexer-multiplexer 54-2 and afurther isolator 55-3 disposed in this order from the input side.Further, a pump source 53-1 is connected to the opticaldemultiplexer-multiplexer 54-1 while a pump source 53-2″ of themodulation polarization multiplexing type is connected to the opticaldemultiplexer-multiplexer 54-2.

The pump source 53-1 produces pump light of, for example, 0.98 μm.Meanwhile, the pump source 53-2″ is formed from a pair of pump sources53-2A″ and 53-2B″, a polarizing multiplexer (PBS) 53-2C″ fororthogonally polarizing and multiplexing pump light from the pumpsources 53-2A″ and 53-2B, and a modulator 53-2D″ for modulating the pumpsources 53-2A and 53-2B with a frequency of several hundreds kHz to 1MHz.

Also in the present modified optical fiber amplifier, the pump sources53-2A″ and 53-2B have an equal pump power and both output pump light of,for example, 1.45 to 1.49 μm (or 1.45 to 1.48 μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 54-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 54-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 45 and having theconstruction described above, pump light from the pump source 53-1 isinputted to one end of the erbium-doped-fiber 51 from the opticaldemultiplexer-multiplexer 54-1 together with signal light. Consequently,the signal light is amplified in the erbium-doped-fiber 51.

Meanwhile, modulated and orthogonally polarized multiplexed pump lighthaving a spectrum of several hundreds kHz or more (the spectral linewidth of the pump light can be widened) is introduced into an output endof the dispersion compensating fiber 52 by way of the opticaldemultiplexer-multiplexer 54-2 to cause Raman amplification to occureffectively in the dispersion compensating fiber 52. Thus, the loss ofthe dispersion compensating fiber 52 is compensated for by such Ramanamplification.

By the construction described above, similar advantages or effects tothose of the fourteenth embodiment described above can be achieved whileraising the threshold level for stimulated Brillouin scattering anddecreasing unfavorable nonlinear effects.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Further, the rare earth doped fiber optical amplification element formedfrom an erbium-doped-fiber may be formed as an optical amplificationelement which has a low noise figure. Or, a Raman optical amplificationelement formed from a dispersion compensating fiber may be disposed as afront stage amplification element while a rare earth doped fiber opticalamplification element formed from an erbium-doped-fiber is disposed as arear stage amplification element.

B15. Fifteenth Embodiment

FIG. 48 is a block diagram showing a fifteenth preferred embodiment ofthe present invention.

Referring to FIG. 48, the optical fiber amplifier shown includes anisolator 125-1, an optical demultiplexer-multiplexer 124-1, anerbium-doped-fiber (rare earth doped fiber) 121-1, another isolator125-2, a silica-type-optical-fiber 122, another erbium-doped-fiber (rareearth doped fiber) 121-2, another optical demultiplexer-multiplexer124-3, and a further isolator 125-3 disposed.

In this order from the input side. A pair of pump sources 123-1 and123-3 for producing pump light of, for example, the 1.47 μm band (1.45to 1.49 μm) are connected to the optical demultiplexer-multiplexers124-1 and 124-3, respectively.

The silica-type-optical-fiber 122 functions as a Raman optical amplifierwhose amplification frequency band can be varied with a pump wavelength.The band characteristic of the silica-type-optical-fiber 122 dependsupon the silica of the host glass and the doping material and theconcentration of the core.

Meanwhile, each of the erbium-doped-fibers 121-1 and 121-2 functions asa rare earth doped fiber optical amplifier whose amplification frequencyband and band characteristic depend upon the host glass and the dopingmaterial of the core.

In the present embodiment, the silica-type-optical-fiber 122 has a smallmode field diameter. Where the noise figure of the Raman opticalamplifier formed from the silica-type-optical-fiber 122 is higher thanthat of the rare earth doped fiber optical amplifiers formed from theerbium-doped-fibers 121-1 and 121-2, one of the rare earth doped fiberoptical amplifier is used as the front stage amplification element andthe Raman optical amplifier is used as the middle stage amplificationelement while the other rare earth doped fiber optical amplifier is usedas the rear stage amplification element in which the signal power ishigh, and they are connected in cascade connection to realize an opticalfiber amplifier which is low in noise and has a flat band characteristicor a wide amplification frequency band.

In particular, by using a rare earth doped fiber optical amplifierhaving a low noise figure (such as an erbium-doped-fiber opticalamplifier pumped with light of the 1.47 μm band) as the front stageamplification element, very low signal light is amplified in a low noisecondition. Further, in order to reduce nonlinear effects whichdeteriorate, the signal to noise ratio (SNR) (here, the “nonlineareffects” signifies effects which deteriorate the signal to noise ratio(SNR) such as self-phase modulation (SPM) of signal light, four wavemixing (FWM), and cross-phase modulation (XPM)), a Raman opticalamplifier for which a silica-type-optical-fiber having a low signalpower is employed is used as the middle stage amplification element.

In the optical fiber amplifier shown in FIG. 48 and having theconstruction described above, pump light from the pump source 123-1 isintroduced into one end of the erbium-doped-fiber 121-1 by way of theoptical demultiplexer-multiplexer 124-1 to pump the erbium-doped-fiber121-1 to amplify signal light. Thereupon, residual pump light isproduced in the erbium-doped-fiber 121-1, and thesilica-type-optical-fiber 122 is pumped with the residual pump light sothat Raman amplification may occur similarly as in a dispersioncompensating fiber.

Meanwhile, pump light from the pump source 123-3 is introduced into anoutput end of the erbium-doped-fiber 121-2 by way of the opticaldemultiplexer-multiplexer 124-3 to pump the erbium-doped-fiber 121-2 toamplify the signal light. Thereupon, residual pump light is produced inthe erbium-doped-fiber 121-2, and the silica-type-optical-fiber 122 ispumped with the residual pump light to cause Raman amplification tooccur.

Since the optical fiber amplifier shown in FIG. 48 employs the pumpsources 123-1 and 123-3 of the 1.47 μm band in this manner, all of theerbium-doped-fibers 121-1 and 121-2 and the silica-type-optical-fiber122 can be pumped. Consequently, the pump source 123-2 in the opticalfiber amplifier shown in FIG. 11 can be omitted. Accordingly, theoptical fiber amplifier is simplified in construction and improved inefficiency of the pump power.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Or, an isolator may be interposed between the silica-type-optical-fiber122 and the erbium-doped-fiber 121-2.

Further, a pump source and an optical demultiplexer-multiplexer for thesilica-type-optical-fiber 122 may be provided additionally.

In particular, similarly as in the optical fiber amplifier of FIG. 11,an optical fiber amplifier may be constructed using pump sources 123-1to 123-3 of the 0.98 μm band and optical demultiplexer-multiplexers124-1 to 124-3.

Furthermore, the silica-type-optical-fiber 122 may be replaced by adispersion compensating fiber.

B15-1. Modification to the Fifteenth Embodiment

FIG. 49 is a block diagram showing a modification to the fifteenthembodiment of the present invention. Referring to FIG. 49, the opticalfiber amplifier shown includes an isolator 125-1, an opticaldemultiplexer-multiplexer 124-1, an erbium-doped-fiber (rare earth dopedfiber) 121-1, another isolator 125-2, a silica-type-optical-fiber 122,an optical filter 126, another erbium-doped-fiber (rare earth dopedfiber) 121-2, another optical demultiplexer-multiplexer 124-3, and afurther isolator 125-3 disposed in this order from the input side. Apair of polarization multiplexing pump sources 123-1′ and 123-3′ areconnected to the optical demultiplexer-multiplexers 124-1 and 124-3,respectively.

The pump source 123-1′ is formed from a pair of pump sources 123-1A′ and123-1B′, and a polarizing multiplexer (PBS) 123-1C′ for orthogonallypolarizing and multiplexing pump light from the pump sources 123-1A′ and123-1B′. The pump sources 123-1A′ and 123-1B′ have an equal pump powerand both output pump light of, for example, 1.45 to 1.49 μm (or 1.45 to1.48 μm).

Meanwhile, the pump source 123-3′ is formed from a pair of pump sources123-3A′ and 123-3B′, and a polarizing multiplexer (PBS) 123-3C′ fororthogonally polarizing and multiplexing pump light from the pumpsources 123-3A′ and 123-3B′. Here, since the pump source 123-3′ isconstructed as a pump source which orthogonally polarizes andmultiplexes pump light in order to merely increase the pump power, thepump wavelengths and the pump powers of the pump sources 123-3A′ and123-3B′ may be different from each other.

Further, in order that a depolarized condition of orthogonally polarizedmultiplexed pump light may be kept also in the silica-type-optical-fiber122, the erbium-doped-fiber 121-1 and the silica-type-optical-fiber 122are either secured firmly to bobbins or like elements or accommodated ina housing so that they may not be influenced by external air and soforth.

It is to be noted that the isolators 125-1 to 125-3 are opticalisolators of the non-polarization dependent type. Further, the opticalfilter 126 is used to remove or level an ASE peak in the proximity of1.535 μm produced in the erbium-doped-fiber 121-1, and it can beomitted.

In the optical fiber amplifier shown in FIG. 49 and having theconstruction described above, pump light of the 1.47 μm band from thepump source 123-1′ is introduced into one end of the erbium-doped-fiber121-1 by way of the optical demultiplexer-multiplexer 124-1 to pump theerbium-doped-fiber 121-1 to amplify signal light. Thereupon,residual-pump light is produced, and the silica-type-optical-fiber 122is pumped with the residual pump light to cause Raman amplification tooccur.

Meanwhile, pump light of 1.47 μm from the pump source 123-3′ isintroduced into an output end of the erbium-doped-fiber 121-2 by way ofthe optical demultiplexer-multiplexer 124-3 to pump theerbium-doped-fiber 121-2 to amplify the signal light. Thereupon,residual pump light is produced. And the silica-type-optical-fiber 122is pumped with the residual pump light to cause Raman amplification tooccur.

In the optical fiber amplifier shown in FIG. 49, by employing the pumpsources 123-1′ and 123-3′ of the 1.47 μm band in this manner, all of theerbium-doped-fibers 121-1 and 121-2 and the silica-type-optical-fiber122 can be pumped. Consequently, the pump source 123-2 in the opticalfiber amplifier shown in FIG. 11 can be omitted. Accordingly, theoptical fiber amplifier is simplified in construction and improved inefficiency of the pump power.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is Inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Further, a pump source and an optical demultiplexer-multiplexer for thesilica-type-optical-fiber 122 may be provided additionally.

In particular, similarly as in the optical fiber amplifier of FIG. 11,an optical fiber amplifier may be constructed using pump sources 123-1to 123-3 of the 0.98 μm band and optical demultiplexer-multiplexers124-1 to 124-3.

Furthermore, an isolator may be interposed between thesilica-type-optical-fiber 122 and the erbium-doped-fiber 121-2.

Furthermore, the silica-type-optical-fiber 122 may be replaced by adispersion compensating fiber.

B11. Sixteenth Embodiment

FIG. 50 is a block diagram showing a sixteenth preferred embodiment ofthe present invention. Referring to FIG. 50, the optical fiber amplifiershown Includes an isolator 115-1, an optical demultiplexer-multiplexer114-1, an erbium-doped-fiber (rare earth doped fiber) 111, anotherisolator 115-2, a silica-type-optical-fiber 112, a polarization keepingoptical demultiplexer-multiplexer 114-2, and a further isolator 115-3disposed in this order from the input side. A pump source 113-1 isconnected to the optical demultiplexer-multiplexer 114-1, and apolarization multiplexing pump source 113-2 is connected to opticaldemultiplexer-multiplexer 114-2.

Thus, in the optical fiber amplifier shown in FIG. 50, the rare earthdoped fiber optical amplifier and the Raman optical amplifier areemployed so as to compensate for each other so that a further flattenedband characteristic or a further widened amplification frequency bandcan be obtained. Then, the rare earth doped fiber optical amplifier(such as an erbium-doped-fiber amplifier pumped with 0.98 μm band orpumped with 1.47 μm) having a low noise figure is used as the frontstage amplification element and the Raman optical amplifier formed froma silica-type-optical-fiber is used as the rear stage amplificationelement, and they are connected in cascade connection so that an opticalfiber amplifier has a low noise characteristic and has a furtherflattened band characteristic or a further widened amplificationfrequency band.

In particular, where the noise figure of the Raman optical amplifier ishigher than that of the rare earth doped fiber optical amplifier, therare earth doped fiber optical amplifier is used as the frontamplification element while the Raman optical amplifier is used as therear stage amplification element and they are connected in cascadeconnection to realize a low noise optical fiber amplifier.

Further, the pump source 113-1 outputs pump light of, for example, 0.98μm. Meanwhile, the pump source 113-2 is formed from a pair of pumpsources 113-2A and 113-2B, and a polarizing multiplexer (PBS) 113-2C fororthogonally polarizing and multiplexing pump light from the pumpsources 113-2A and 113-2B.

Also in the present optical fiber amplifier, the pump sources 113-2A and113-2B have an equal pump power and both output pump light of, forexample, 1.45 to 1.49 μm (or 1.45 to 1.48 μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 114-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 114-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 50 and having theconstruction described above, pump light from the pump source 113-1 isinputted to one end of the erbium-doped-fiber 111 by way of the opticaldemultiplexer-multiplexer 114-1 together with signal light.Consequently, the signal light is amplified in the erbium-doped-fiber111.

Meanwhile, orthogonally polarized multiplexed pump light is introducedinto an output end of the silica-type-optical-fiber 112 by way of theoptical demultiplexer-multiplexer 114-2 to cause Raman amplification tooccur effectively in the silica-type-optical-fiber 112. Thus, the lossof the silica-type-optical-fiber 112 is compensated for by such Ramanamplification.

Also by the construction described above, similar advantages or effectsto those of the fourteenth embodiment described above can be achieved.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Alternatively, a single pump source which produces pump light of the1.47 μm band may be provided so that it may serve as both of the pumpsource for the silica-type-optical-fiber and the pump source for theerbium-doped-fiber.

On the other hand, where a high output cannot be obtained from the Ramanoptical amplifier, a Raman optical amplifier formed from asilica-type-optical-fiber or a dispersion compensating fiber is used asthe amplification element on the input side (front stage amplificationelement) while a rare earth doped fiber optical amplifier formed from anerbium-doped-fiber is used as the amplification element on the outputside (rear stage amplification element), and they are connected incascade connection.

Particularly, where the pump wavelength of the pump source for the Ramanoptical amplifier is approximately 1.44 μm, the concave of the gainwhich appears in the proximity of approximately 1.54 μm of the rareearth doped fiber optical amplifier can be compensated for by Ramanoptical amplification. On the hand, where the pump wavelength of thepump source for the Raman optical amplifier is approximately 1.46 μm, adecrease in gain which occurs in the longer wavelength side of the rareearth doped fiber optical amplifier than approximately 1.57 μm can becompensated for by the Raman optical amplification. Consequently,further leveling or widening of the band characteristic of the opticalfiber amplifier can be achieved.

Further, the optical fiber amplifier can be constructed in the followingmanner so that it may have a further flattened band characteristic or afurther wider amplification frequency band. In particular, in order toreduce the pump power (threshold pump power) at which a Raman opticalamplifier for which a silica-type-optical-fiber or a dispersioncompensating fiber is used begins to produce a gain, asilica-type-optical-fiber having a reduced mode field diameter is used,and in order to reduce an influence of nonlinear effects which increasesas a result of the reduction of the mode field diameter, a Raman opticalamplifier formed from a silica-type-optical-fiber is employed as theamplification element on the input side (front stage amplificationelement) in which the signal power is low while a rare earth doped fiberoptical amplifier formed from an erbium-doped-fiber is used as theamplification element on the output side (rear stage amplificationelement) in which the signal power is high, and they are connected incascade connection.

B16-1. First Modification to the Sixteenth Embodiment

FIG. 51 is a block diagram showing a first modification to the sixteenthembodiment of the present Invention. Referring to FIG. 51, the opticalfiber amplifier shown includes an isolator 115-1, an opticaldemultiplexer-multiplexer 114-1, an erbium-doped-fiber (rare earth dopedfiber) 111, another isolator 115-2, a silica-type-optical-fiber 112, apolarization keeping optical demultiplexer-multiplexer 114-2, and afurther isolator 115-3 disposed in this order from the input side. Apump source 113-1 is connected to the optical demultiplexer-multiplexer114-1, and a depolarizing polarization multiplexing pump source 113-2′is connected to the optical demultiplexer-multiplexer 114-2.

The pump source 113-1 outputs pump light of, for example, 0.98 μm. Thepump source 113-2′ is formed from a single pump source 113-2A′, and adepolarizer 113-2B′ for depolarizing pump light from the pump source113-2A′.

The depolarizer 113-2B′ reduces the polarization dependency of a Ramanoptical amplifier formed from the silica-type-optical-fiber 112. Thedepolarizer 113-2B′ is formed from a polarization keeping coupler113-2E′ for demultiplexing pump light from the pump source 113-2A′, anda polarizing multiplexer (PBS) 113-2C′ for orthogonally polarizing andmultiplexing the pump light demultiplexed by the polarization keepingcoupler 113-2E′ and the pump light delayed by a delay line.

Also in the modified optical fiber amplifier, the pump source 113-2A′outputs pump light of, for example, 1.45 to 1.49 μm (or 1.45 to 1.48μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 114-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 114-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 51 and having theconstruction described above, pump light from the pump source 113-1 isinputted to one end of the erbium-doped-fiber 111 by way of the opticaldemultiplexer-multiplexer 114-1 together with signal light.Consequently, the signal light is amplified in the erbium-doped-fiber111.

Meanwhile, depolarized pump light from the pump source 113-2′ isintroduced into an output end of the silica-type-optical-fiber 112 byway of the optical demultiplexer-multiplexer 114-2 to cause Ramanamplification to occur effectively in the silica-type-optical-fiber 112.Thus, the loss of the silica-type-optical-fiber 112 is compensated forby such Raman amplification.

Also by the construction described above, similar advantages or effectsto those of the sixteenth embodiment described above can be achievedwhile decreasing the polarization dependency of thesilica-type-optical-fiber 112.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Alternatively, a single pump source which produces pump light of the1.47 μm band may be provided so that it may serve as both of the pumpsource for the silica-type-optical-fiber and the pump source for theerbium-doped-fiber.

B16-2. Second Modification to the Sixteenth Embodiment

FIG. 52 is a block diagram showing a second modification to thesixteenth embodiment of the present invention. Referring to FIG. 52, theoptical fiber amplifier shown includes an isolator 115-1, an opticaldemultiplexer-multiplexer 114-1, an erbium-doped-fiber (rare earth dopedfiber) 111, another isolator 115-2, a silica-type-optical-fiber 112, apolarization keeping optical demultiplexer-multiplexer 114-2, and afurther isolator 115-3 disposed in this order from the input side. Apump source 113-1 is connected to the optical demultiplexer-multiplexer114-1, and a modulating polarization multiplexing pump source 113-2″ isconnected to optical demultiplexer-multiplexer 114-2.

The pump source 113-1 outputs pump light of, for example, 0.98 μm. Thepump source 113-2″ is formed from a pair of pump sources 113-2A″ and113-2B″, a polarizing multiplexer (PBS) 113-2C″ for orthogonallypolarizing and multiplexing pump light from the pump sources 113-2A″ and113-2B″, and a modulator 113-2D″ for modulating the pump sources 113-2A″and 113-2B″ with a frequency of several hundreds kHz to 1 MHz.

Also in the modified optical fiber amplifier, the pump sources 113-2A″and 113-2B″ have an equal pump power and both output pump light of, forexample, 1.45 to 1.49 μm (or 1.45 to 1.48 μm).

It is to be noted that an optical demultiplexer-multiplexer of thefusion type which has no polarization keeping function is used for theoptical demultiplexer-multiplexer 114-1 while another opticaldemultiplexer-multiplexer of the optical film type is used for theoptical demultiplexer-multiplexer 114-2 so that multiplexing ordemultiplexing of light may be performed while keeping polarizationconditions of the light.

In the optical fiber amplifier shown in FIG. 52 and having theconstruction described above, pump light from the pump source 113-1 isinputted to one end of the erbium-doped-fiber 111 by way of the opticaldemultiplexer-multiplexer 114-1 together with signal light.Consequently, the signal light is amplified in the erbium-doped-fiber111.

Meanwhile, modulated and orthogonally polarized multiplexed pump lighthaving a spectrum of several hundreds kHz or more (the spectral linewidth of the pump light can be widened) from the pump source 113-2″ isintroduced into an output end of the silica-type-optical-fiber 112 byway of the optical demultiplexer-multiplexer 114-2 to cause Ramanamplification to occur effectively in the silica-type-optical-fiber 112.Thus, the loss of the silica-type-optical-fiber 112 is compensated forby such Raman amplification.

By the construction described above, similar advantages or effects tothose of the sixteenth embodiment described above can be achieved whileraising the threshold level for stimulated Brillouin scattering anddecreasing unfavorable nonlinear effects.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is Inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Alternatively, a single pump source which produces pump light of the1.47 μm band may be provided so that it may serve as both of the pumpsource for the silica-type-optical-fiber and the pump source for theerbium-doped-fiber.

B17. Seventeenth Embodiment

FIG. 55 is a block diagram showing a seventeenth preferred embodiment ofthe present invention. Referring to FIG. 55, the optical fiber amplifiershown includes an isolator 65-1, an optical demultiplexer-multiplexer64, an erbium-doped-fiber (rare earth doped fiber amplification element)61, a dispersion compensating fiber (optical fiber attenuation element)62, and another isolator 65-3 disposed in this order from the inputside. A pump source 63 is connected to the opticaldemultiplexer-multiplexer 64.

The pump source 63 produces pump light, for example, of the 1.47 μm band(1.45 to 1.49 μm).

A rare earth doped fiber optical amplifier having a high gain sometimessuffers from unnecessary oscillations which are produced when itperforms optical amplification. If such unnecessary oscillations areproduced, the rare earth doped fiber optical amplifier operates butunstably.

For example, in an erbium-doped-fiber optical amplifier, spontaneousemission light (ASE) of 1.53 to 1.57 μm in wavelength is produced whenoptical amplification is performed, and since the ASE is repetitivelyreflected at reflection points in the erbium-doped-fiber opticalamplifier, unnecessary oscillations are liable to be produced.Particularly with an erbium-doped-fiber optical amplifier adjusted formultiple wavelength collective amplification (that is, anerbium-doped-fiber optical amplifier having a high pump rate), since ithas a high gain in the proximity of 1.53 μm, unnecessary oscillationsare liable to be produced at this wavelength. When such unnecessaryoscillations are produced, the erbium-doped-fiber optical amplifieroperates unstably.

In order to suppress such unstable operation, it is effective to providea medium (which is called loss medium) for causing signal light to loseits power (for attenuating signal light) (the principle will behereinafter described).

In such an optical fiber amplifier as shown in FIG. 55, the dispersioncompensating fiber 62 is pumped with remaining pump light introducedinto it through the erbium-doped fiber 61 to compensate for signal lightagainst the loss (attenuation) caused by the dispersion compensatingfiber 62. Actually, however, it is difficult to compensate against theoverall loss and some loss remains, and accordingly, the dispersioncompensating fiber 62 functions as a loss medium.

Here, the principle of suppression of unstable operation arising fromthe provision of a loss medium will be described.

Generally, where the gain of an erbium-doped-fiber is represented by G,the reflectivities at the opposite ends (front end and rear end) of theerbium-doped-fiber are represented by R1 and R2 (here, the reflectivityR1 is a reflectivity in reflection from all parts located forwardly ofthe front end of the erbium-doped-fiber, and the reflectivity R2 is areflectivity in reflection from all parts located rearwardly of the rearend of the erbium-doped-fiber), and the geometrical mean of R1 and R2 isrepresented by R (R=(R1R2)^(1/2)), GR can be regarded as a parameterindicating the degree of stability of operation of theerbium-doped-fiber. When GR is high, the erbium-doped-fiber operatesunstably, and particularly when GR is higher than 1, oscillations areproduced in the erbium-doped-fiber. Therefore, GR must be low, andparticularly, GR is set lower than 0.02 as a target.

If the dispersion compensating fiber 62 (whose loss is represented by η(0≦η≦1)) is provided at the following stage (output side of signallight) to the erbium-doped-fiber 61 (whose gain is represented by G),for example, by fusion connection, then an interface A appears betweenthe erbium-doped-fiber 61 and the dispersion compensating fiber 62 asseen in FIG. 55.

In this instance, as seen in FIG. 55, the reflectivity at the rear endof the erbium-doped-fiber 61 is represented by R1 and the reflectivityat the front end of the dispersion compensating fiber 62 is representedby R2 (here, the reflectivity R1 is a reflectivity in reflection fromall parts located forwardly of the front end of the erbium-doped-fiber61, and the reflectivity R2 is a reflectivity in reflection from allparts located rearwardly of the rear end of the dispersion compensatingfiber 62). Further, where the reflectivity in reflection caused by adifference in reflectivity at the interface A between theerbium-doped-fiber 61 and the dispersion compensating fiber 62 isrepresented by RA (RA<<R1, R2; this condition is satisfied where theloss medium is an optical fiber), the parameter indicating the degree ofstability of operation of the erbium-doped-fiber changes from CR to(Gη)R. In other words, CR is considered to be a gain in one way whenlight takes a round. Where a loss medium Is provided, since the net gainwhen light takes a round Is given by (R1×G×η)×(R2×η>C)=(Gη)²R1R2, thenet gain in one way is given by Gη(R1R2)^(1/2)=(Gη)R. It is to be notedthat, since RA<<R1, R2, the influence of the reflectivity RA can beignored. Here, since 0≦η≦1, GR is equivalently low.

Since the parameter GR indicating the degree of stability of operationof the erbium-doped-fiber becomes low by the provision of a loss mediumin this manner, unstable operation of the erbium-doped-fiber 61 can besuppressed.

In the optical fiber amplifier according to the present embodiment, bypumping the dispersion compensating fiber 62 provided at the followingstage to the erbium-doped-fiber 61 as shown in FIG. 55 with residualpump light from the erbium-doped-fiber 61, the dispersion compensatingfiber 62 is compensated for against the loss (including leveling of theconcave of the gain of the erbium-doped-fiber 61 and compensationagainst the reduction of the gain of the erbium-doped-fiber 61) andunstable operation of the erbium-doped-fiber 61 is simultaneouslysuppressed by the remaining loss.

In the optical fiber amplifier shown in FIG. 55 and having theconstruction described above, pump light is introduced into one end ofthe erbium-doped-fiber 61 from the optical demultiplexer-multiplexer 64to pump the erbium-doped-fiber 61 to amplify signal light. Consequently,residual pump light arrives at the other end of the erbium-doped-fiber61. Thereafter, the residual pump light is supplied to the dispersioncompensating fiber 62 so that Raman amplification may occur in thedispersion compensating fiber 62.

The reason why signal light can be amplified by both of theerbium-doped-fiber and the dispersion compensating fiber using thecommon pump source to them is such as follows.

In particular, the pump wavelength band when signal light of the 1.55 μmband is Raman amplified is the 1.47 μm band (1.45 to 1.49 μm) which isthe pump wavelength band of the erbium-doped-fiber (EDF), andaccordingly, Raman amplification can be caused to occur using residualpump power when the EDF is pumped with light of the 1.47 μm band. Fromthis reason, while optical amplification is performed by theerbium-doped-fiber 61, the dispersion compensating fiber 62 can becompensated for against the loss.

Consequently, similarly as in the seventh embodiment describedhereinabove, a wide bandwidth optical amplifier wherein the unevennessof the wavelength characteristic of the erbium-doped-fiber amplifier isleveled can be realized, and the wide bandwidth optical amplifier can besuitably applied to multiple wavelength collective amplification.Further, since the single pump source is involved, the optical fiberamplifier can be constructed in simplified structure and at a reducedcost.

Further, in the optical fiber amplifier, suppression of unstableoperation of the erbium-doped-fiber 61 by means of the loss of thedispersion compensating fiber 62 is achieved simultaneously.Consequently, unnecessary oscillating operation of a rare earth dopedfiber optical amplifier adjusted for wavelength multiplexing (WDM) canbe prevented to achieve stabilized optical amplification.

It is to be noted that, where the pump source 63 generates pump light of0.98 μm, the dispersion compensating fiber 62 does not perform Ramanamplification, and accordingly, compensation against the loss of thedispersion compensating fiber 62 does not take place.

It is also to be noted that the reflectivity of the dispersioncompensating fiber due to Rayleigh backscattering is ignored in theabove discussion. The reflectivity depends on the length of thedispersion compensating fiber. Therefore, if the reflectivity cannot beignored, an optical isolator should be added to the configuration shownin FIG. 55, for example, between the erbium-doped-fiber 61 and thedispersion compensating fiber 62. The addition of an optical Isolator isnormally effective where the Rayleigh backscattering cannot be ignored.

Also the optical fiber amplifier of the present embodiment may bemodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions of the opticalfiber amplifier, input signal light is inputted by way of an opticalcirculator and output signal light is outputted by way of the opticalcirculator in a similar manner as In the arrangement shown in FIGS. 18or 30.

Further, the pump source 63 may alternatively be formed from two pumpsources and a polarizing multiplexer which orthogonally polarizes andmultiplexes pump light from the pump sources or may otherwise be formedfrom a combination of a pump source and a depolarizer by means of whichpump light is depolarized or else may generate modulated pump light.

B17-1. First Modification to the Seventeenth Embodiment

FIG. 56 is a block diagram showing a first modification to theseventeenth embodiment of the present invention. Referring to FIG. 56,the optical fiber amplifier shown includes an isolator 115-1, an opticaldemultiplexer-multiplexer 114-1, an erbium-doped-fiber (rare earth dopedfiber amplification element) 111, a silica-type-optical-fiber (opticalfiber attenuation element) 112, and another isolator 115-3 disposed inthis order from the input side. A pump source 113-1 is connected to theoptical demultiplexer-multiplexer 114-1.

Further, the pump source.113-1 outputs pump light of, for example, the1.47 μm band (1.45 to 1.49 μm). Meanwhile, an opticaldemultiplexer-multiplexer, for example, of the fusion connection type isemployed for the optical demultiplexer-multiplexer 114-1.

As described hereinabove in connection with the seventeenth embodiment,a rare earth doped fiber optical amplifier having a high gain sometimessuffers from unnecessary oscillations which are produced when itperforms optical amplification, and if such unnecessary oscillations areproduced, the rare earth doped fiber optical amplifier operatesunstably.

Therefore, also in the optical fiber amplifier shown in FIG. 56,similarly as in the optical fiber amplifier shown in FIG. 55, thesilica-type-optical-fiber 112 as a loss medium is provided at thefollowing stage to the erbium-doped-fiber 111 as a rare earth dopedfiber optical amplifier so as to suppress unstable operation of theerbium-doped-fiber 111. It is to be noted that, also in FIG. 56,reference characters R1, R2 and RA represent reflectivities, and Arepresents an interface.

Similarly as in the seventeenth embodiment described above, in theoptical fiber amplifier shown in FIG. 56, by pumping thesilica-type-optical-fiber 112 provided at the following stage to theerbium-doped-fiber 111 with residual pump light from theerbium-doped-fiber 111, the silica-type-optical-fiber 112 is compensatedfor against the loss (Including leveling of the concave of the gain ofthe erbium-doped-fiber 111 and compensation against the reduction of thegain of the erbium-doped-fiber 111) and unstable operation of theerbium-doped-fiber 111 is simultaneously suppressed by the remainingloss.

In the optical fiber amplifier shown in FIG. 56 and having theconstruction described above, pump light from the pump source 113-1 isinputted to one end of the erbium-doped-fiber 111 by way of the opticaldemultiplexer-multiplexer 114-1 together with signal light.Consequently, the signal light is amplified in the erbium-doped-fiber111.

Further, residual pump light which is produced in this instance is usedto pump the silica-type-optical-fiber 112 so as to perform Ramanamplification similarly as in a dispersion compensating fiber, and thesilica-type-optical-fiber 112 is compensated for against the loss by theRaman amplification.

In this manner, in the optical fiber amplifier shown in FIG. 56, byemploying the pump source 113-1 of the 1.47 μm band, both of theerbium-doped-fiber 111 and the silica-type-optical-fiber 112 can bepumped. Consequently, simplification of an optical fiber amplifier andimprovement in efficiency of the pump power can be achieved.

Further, in the optical fiber amplifier, removal of unnecessaryoscillations originating in the erbium-doped-fiber 111 by means of theloss of the silica-type-optical-fiber 112 is achieved simultaneously.Consequently, unnecessary oscillating operation of a rare earth dopedfiber optical amplifier adjusted for wavelength multiplexing (WDM) canbe prevented to achieve stabilized optical amplification.

It is to be noted that, where the pump source 113-1 generates pump lightof 0.98 μm, the silica-type-optical-fiber 112 does not perform Ramanamplification, and accordingly, the silica-type-optical-fiber 112 is notcompensated for against the loss.

It is also to be noted that the reflectivity of the dispersioncompensating fiber due to Rayleigh backscattering is ignored in theabove discussion. The reflectivity depends on the length of thedispersion compensating fiber. Therefore, if the reflectivity cannot beignored, an optical isolator should be added to the configuration shownin FIG. 56, for example, between the erbium-doped-fiber 111 and thesilica-type-optical-fiber 122. The addition of an optical isolator isnormally effective where the Rayleigh backscattering cannot be ignored.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions, input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

B17-2. Second Modification to the Seventeenth Embodiment

FIG. 57 is a block diagram showing a second modification to theseventeenth embodiment of the present invention. Referring to FIG. 57,the optical fiber amplifier shown includes an isolator 65-1, an opticaldemultiplexer-multiplexer 64-1, an erbium-doped-fiber (front stageoptical amplification element formed as a rare earth doped fiberamplification element) 61-1, a dispersion compensating fiber (opticalfiber attenuation element) 62, another erbium-doped-fiber (rear stageoptical amplification element formed as a rare earth doped fiberamplification element) 61-2, another optical demultiplexer-multiplexer64-2 and another isolator 65-3 disposed in this order from the inputside. A pump source 63-1 is connected to the opticaldemultiplexer-multiplexer 64-1, and another pump source 63-2 isconnected to the optical demultiplexer-multiplexer 64-2.

The pump sources 63-1 and 63-2 both generate pump light of, for example,the 1.47 μm band (1.45 to 1.49 μm).

As described hereinabove in connection with the seventeenth embodiment,a rare earth doped fiber optical amplifier having a high gain sometimessuffers from unnecessary oscillations which are produced when itperforms optical amplification, and if such unnecessary oscillations areproduced, the rare earth doped fiber optical amplifier operatesunstably.

In the optical fiber amplifier of the seventeenth embodiment shown inFIG. 55, the dispersion compensating fiber 62 as a loss medium isprovided at the following stage to the erbium-doped-fiber 61 as a rareearth doped fiber optical amplifier so that unstable operation of theerbium-doped-fiber 61 is suppressed.

However, where the gain G of the erbium-doped-fiber 61 is very high,since the GR parameter defined by the reflectivity R1, the gain G andthe reflectivity RA exhibits a high value (since the gain G of theerbium-doped-fiber 61 is very high, although RA<<R1, R2, an influence ofthe reflectivity RA cannot be ignored), even if the dispersioncompensating fiber 62 is provided at the following stage to theerbium-doped-fiber 61, the effect of the loss η of it does not appear,and unstable operation of the erbium-doped-fiber 61 cannot besuppressed.

Thus, in order to suppress unstable operation of the erbium-doped-fiber61 also in such an instance, the erbium-doped-fiber 61 is divided intofront and rear stage erbium-doped-fibers, between which the dispersioncompensating fiber 62 is disposed, thereby obtaining the optical fiberamplifier shown in FIG. 57.

The principle of suppression of unstable operation in this instance willbe described below with reference to FIG. 57.

If the dispersion compensating fiber 62 (whose loss is represented byη(0≦η≦1)) is provided between the erbium-doped-fibers 61-1 and 61-2(whose gains are given by G/2), for example, by fusion connection, thenan interface A′ appears between the erbium-doped-fiber 61-1 and thedispersion compensating fiber 62 and another interface B′ appearsbetween the dispersion compensating fiber 62 and the erbium-doped-fiber61-2 as seen in FIG. 57.

The reflectivity at the front end of the erbium-doped-fiber 61-1 isrepresented by R1′ and the reflectivity at the rear end of theerbium-doped-fiber 61-2 is represented by R2′, the reflectivity at theinterface A′ is represented by RA′ (RA′<<R1′, R2′), and the reflectivityat the interface B′ is presented by RB′ (RB′<<R1′, R2′). Thereflectivity R1′ is a reflectivity in reflection from all parts locatedforwardly of the front end of the erbium-doped-fiber 61-1, and thereflectivity R2′ is a reflectivity in reflection from all parts locatedrearwardly of the rear end of the erbium-doped-fiber 61-2. Further, thereflectivity RA′ is a reflectivity in reflection caused by a differencein reflectivity at the interface A′, and the reflectivity RB′ is areflectivity in reflection caused by a difference in reflectivity at theinterface B′.

In this instance, the following GR parameters are applicable. Inparticular, (1) a GR parameter defined by the reflectivity R1′, the gainG/2 of the erbium-doped-fiber 61-1 and the reflectivity RA′, (2) anotherGR parameter defined by the reflectivity R1′, the gain G/2 of theerbium-doped-fiber 61-1, the loss η and the reflectivity RB′, (3) afurther GR parameter defined by the reflectivity R1′, the gain G/2 ofthe erbium-doped-fiber 61-1, the loss η, the gain G/2 of theerbium-doped-fiber 61-2 and the reflectivity R2′, (4) a still further GRparameter defined by the reflectivity RA′, the loss A, the gain G/2 ofthe erbium-doped-fiber 161-2 and the reflectivity R2′, and (5) a yetfurther GR parameter defined by the reflectivity RB′, the gain G/2 ofthe erbium-doped-fiber 61-2 and the reflectivity R2′.

In regard to the GR parameter of (1), with the erbium-doped-fiber 61shown in FIG. 55, since the gain of it is G, GR=G(R1RA)^(1/2), but withthe erbium-doped-fiber 61-1 shown in FIG. 57, since the gain of it isG/2 and equal to one half the gain G of the erbium-doped-fiber 61 shownin FIG. 55, GR=(G/2)(R1RA)^(1/2) (RA′=RA) and is equal to one half theGR value of the erbium-doped-fiber 61 shown in FIG. 55.

In regard to the GR parameter of (2), with the erbium-doped-fiber 61-1,since the loss η(0≦η≦1) is present at the following stage to it, the netgain when light takes a round is, similarly as in the seventeenthembodiment, [R1′×(G/2)×η]×[RB′×1×G/2)]=[(G/2)η]²R1′RB′, andconsequently, the net gain in one way is (G/2)η(R1′RB′)^(1/2). Here,since 0≦η≦1 and RB′=RB, GR is equivalently low. Further, since RA′≅RB′,the GR parameter exhibits a further lower value than that of (1), and GRin this instance can be ignored.

In regard to the GR parameter of (3), since the loss η(0≦η≦1) is presentbetween the erbium-doped-fibers 61-1 and 61-2, the net gain when lighttakes a round is given by, similarly as in the seventeenth embodiment,[R1′×(G/2)×η]×[R2′×η×(G/2)]=[(G/2)η]²R1′R2′, and consequently, the netgain in one way is (G/2)η(R1′R2′)^(1/2)=[(G/2)η]R, and the parameterindicating the degree of stability of operation of theerbium-doped-fibers 61-1 and 61-2 changes from (G/2)R to [(G/2)η]R. Itis to be noted that, since RA′<<R1′, R2′ and RB′<<R1′, R2′, theinfluence of the reflectivity RA′ and the reflectivity RB′ can beignored. Here, since 0≦η≦1, GR is equivalently low.

It is to be noted that the GR parameters of (4) and (5) are similar tothose of the parameters of (2) and (1), respectively.

Accordingly, when the gain G of the erbium-doped-fiber 61 shown in FIG.55 is very high, since the GR parameter defined by R1, G and RA is veryhigh, the erbium-doped-fiber 61 operates unstably, but where theerbium-doped-fiber 61 is divided into the erbium-doped-fibers 61-1 and61-2 at the preceding and following stages as seen in FIG. 57 and thedispersion compensating fiber 62 as a loss medium is disposed betweenthe erbium-doped-fibers 61-1 and 61-2, the GR parameters of (1) and (5)can be made low, and consequently, unstable operation of theerbium-doped-fibers 61-1 and 61-2 can be suppressed.

Therefore, in the optical fiber amplifier shown in FIG. 57, by pumpingthe dispersion compensating fiber 62 interposed between theerbium-doped-fibers 61-1 and 61-2 with residual pump light from theerbium-doped-fibers 61-1 and 61-2, the dispersion compensating fiber 62is compensated for against the loss (including leveling of the concavesof the gains of the erbium-doped-fibers 61-1 and 61-2 and compensationagainst the reduction of the gains of the erbium-doped-fibers 61-1 and61-2) and unstable operation of the erbium-doped-fibers 61-1 and 61-2 issimultaneously suppressed by the remaining losses.

In the optical fiber amplifier shown in FIG. 57 and having theconstruction described above, pump light is inputted to one end of theerbium-doped-fiber 61-1 by way of the optical demultiplexer-multiplexer64-1 together with signal light and pumps the erbium-doped-fiber 61-1 toamplify the signal light. Residual pump light which is produced in thisinstance arrives at the other end of the erbium-doped-fiber 61-1. Theresidual pump light is supplied into the dispersion compensating fiber62 to cause Raman amplification to occur.

Meanwhile, another pump light is introduced into an output end of theerbium-doped-fiber 61-2 by way of the optical demultiplexer-multiplexer64-2 to pump the erbium-doped-fiber 61-2 to amplify the signal lightinputted into the input end of the erbium-doped-fiber 61-2. Also in thisinstance, residual pump light arrives at the other end of theerbium-doped-fiber 61-2. The residual pump light is supplied to thedispersion compensating fiber 62 so that Raman amplification may occurin the dispersion compensating fiber 62.

In this instance, since the dispersion compensating fiber 62 causesRaman amplification to occur using the residual pump light from theerbium-doped-fibers 61-1 and 61-2 on the front and rear sides, thedispersion compensating fiber 62 exhibits a higher compensation effectas much. Consequently, a wide bandwidth optical amplifier can berealized while achieving simplification in structure and reduction incost.

Further, in the optical fiber amplifier, removal of unnecessaryoscillations produced in the erbium-doped-fibers 61-1 and 61-2 by meansof the loss of the dispersion compensating fiber 62 is simultaneouslyachieved. Consequently, unnecessary oscillating operation of a rareearth doped fiber optical amplifier adjusted for wavelength multiplexing(WDM) can be prevented to achieve stabilized optical amplification in areduced noise condition.

It is to be noted that, where the pump sources 63-1 and 63-2 generatepump light of 0.98 μm, the dispersion compensating fiber 62 does notperform Raman amplification, and accordingly, the dispersioncompensating fiber 62 is not compensated for against the loss.

It is also to be noted that the reflectivity of the dispersioncompensating fiber due to Rayleigh backscattering is ignored in theabove discussion. The reflectivity depends on the length of thedispersion compensating fiber. Therefore, if the reflectivity cannot beignored, an optical isolator should be added to the configuration shownin FIG. 57, for example, between the erbium-doped-fiber 61-1 and thedispersion compensating fiber 62. The addition of an optical Isolator isnormally effective where the Rayleigh backscattering cannot be ignored.

Also the present modified optical fiber amplifier may be furthermodified such that, in place of the provision of an isolator at theinput portion or at both of the input and output portions, input signallight is inputted by way of an optical circulator and output signallight is outputted by way of the optical circulator in a similar manneras in the arrangement shown in FIGS. 18 or 30.

Further, a pump source and an optical demultiplexer-multiplexer for thedispersion compensating fiber 62 may be provided additionally. Inparticular, similarly as in the optical fiber amplifier of FIG. 12, anoptical fiber amplifier may be constructed using pump sources 133-1 to133-3 and optical demultiplexer-multiplexers 134-1 to 134-3.

Furthermore, a silica-type-optical-fiber may be employed in place of thedispersion compensating fiber 62.

B17-3. Third Modification to the Seventeenth Embodiment

FIG. 58 is a block diagram showing a third modification to theseventeenth embodiment of the present invention. Referring to FIG. 58,the optical fiber amplifier shown includes an isolator 125-1, an opticaldemultiplexer-multiplexer 124-1, an erbium-doped-fiber (front stageoptical amplification element constructed as a rare earth doped fiberamplification element) 121-1, a silica-type-optical-fiber (optical fiberattenuation element) 122, another erbium-doped-fiber (rear stage opticalamplification element constructed as a rare earth doped fiberamplification element) 121-2, another optical demultiplexer-multiplexer124-3, and another isolator 125-3 disposed In this order from the inputside. A pair of pump sources 123-1 and 123-3 for producing pump lightof, for example, the 1.47 μm band (1.45 to 1.49 μm) are connected to theoptical demultiplexer-multiplexers 124-1 and 124-3, respectively.

As described hereinabove in connection with the seventeenth embodiment,a rare earth doped fiber optical amplifier having a high gain sometimessuffers from unnecessary oscillations which are produced when itperforms optical amplification, and if such unnecessary oscillations areproduced, the rare earth doped fiber optical amplifier operatesunstably.

In the optical fiber amplifier shown in FIG. 56, thesilica-type-optical-fiber 122 as a loss medium is provided at thefollowing stage to the erbium-doped-fiber 111 as a rare earth dopedfiber optical amplifier so that unstable operation of theerbium-doped-fiber 111 is suppressed.

However, where the gain C of the erbium-doped-fiber 111 is very high,since the GR parameter exhibits a high value similarly as in the opticalfiber amplifier shown in FIG. 55, even if the silica-type-optical-fiber122 is provided at the following stage to the erbium-doped-fiber 111,the effect of the loss η of it does not appear, and unstable operationof the erbium-doped-fiber 111 cannot be suppressed.

Thus, in order to suppress unstable operation of the erbium-doped-fiber111 also in such an instance, the erbium-doped-fiber 111 is divided intofront and rear stage erbium-doped-fibers, between which thesilica-type-optical-fiber 122 is disposed, thereby obtaining the opticalfiber amplifier shown in FIG. 58. It is to be noted that the principleof suppression of unstable operation in this instance is similar to thatdescribed hereinabove in connection with the second modification to theseventeenth embodiment. Also in FIG. 58, reference characters R1′, R2′,RA′ and RB′ denote each a reflectivity, and A′ and B′ represent each aninterface.

Consequently, in the optical fiber amplifier shown in FIG. 58, bypumping the silica-type-optical-fiber 122 provided at a middle stagewith residual pump light from the erbium-doped-fibers 121-1 and 121-2,the silica-type-optical-fiber 122 is compensated for against the loss(including leveling of the concaves of the gains of theerbium-doped-fibers 121-1 and 121-2 and compensation against thereduction of the gains of the erbium-doped-fibers 121-1 and 121-2) andunstable operation of the erbium-doped-fibers 121-1 and 121-2 issuppressed by the remaining losses simultaneously.

In the optical fiber amplifier shown in FIG. 58 and having theconstruction described above, pump light is introduced into one end ofthe erbium-doped-fiber 121-1 by way of the opticaldemultiplexer-multiplexer 124-1 to pump the erbium-doped-fiber 121-1 toamplify signal light. Thereupon, residual pump light is produced in theerbium-doped-fiber 121-1, and the silica-type-optical-fiber 122 ispumped with the residual pump light so that Raman amplification mayoccur similarly as in a dispersion compensating fiber.

Meanwhile, another pump light is introduced into an output end of theerbium-doped-fiber 121-2 by way of the optical demultiplexer-multiplexer124-3 to pump the erbium-doped-fiber 121-2 to amplify the signal light.Thereupon, residual pump light is produced in the erbium-doped-fiber121-2, and the silica-type-optical-fiber 122 is pumped with the residualpump light to cause Raman amplification to occur.

Since the optical fiber amplifier shown in FIG. 58 employs the pumpsources 123-1 and 123-3 of the 1.47 μm band in this manner, all of theerbium-doped-fibers 121-1 and 121-2 and the silica-type-optical-fiber122 can be pumped. Consequently, the pump source 123-2 in the opticalfiber amplifier shown in FIG. 11 can be omitted. Accordingly, theoptical fiber amplifier is simplified in construction and improved inefficiency of the pump power.

Further, in the optical fiber amplifier, removal of unnecessaryoscillation originating in the erbium-doped-fibers 121-1 and 121-2 bythe loss of the silica-type-optical-fiber 122 is achievedsimultaneously. Consequently, unnecessary oscillating operation of arare earth doped fiber optical amplifier adjusted for wavelengthmultiplexing (WDM) can be prevented to achieve stabilized opticalamplification in a reduced noise condition.

It is to be noted that, where the pump sources 123-1 and 123-3 generatepump light of 0.98 μm, the silica-type-optical-fiber 122 does notperform Raman amplification, and accordingly, thesilica-type-optical-fiber 122 is not compensated for against the loss.

It is also to be noted that the reflectivity of the dispersioncompensating fiber due to Rayleigh backscattering is ignored in theabove discussion. The reflectivity depends on the length of thedispersion compensating fiber. Therefore, if the reflectivity cannot beignored, an optical isolator should be added to the configuration shownin FIG. 58, for example, between the erbium-doped-fiber 121-1 and thesilica-type-optical-fiber 122. The addition of an optical isolator isnormally effective where the Rayleigh backscattering cannot be ignored.

Also the present modified optical fiber amplifier may be modified suchthat, in place of the provision of an isolator at the input portion orat both of the input and output portions input signal light is inputtedby way of an optical circulator and output signal light is outputted byway of the optical circulator in a similar manner as in the arrangementshown in FIGS. 18 or 30.

Or, an isolator may be interposed between the silica-type-optical-fiber122 and the erbium-doped-fiber 121-2.

Further, a pump source and an optical demultiplexer-multiplexer for thesilica-type-optical-fiber 122 may be provided additionally. Inparticular, similarly as in the optical fiber amplifier of FIG. 11, anoptical fiber amplifier may be constructed using pump sources 123-1 to123-3 and optical demultiplexer-multiplexers 124-1 to 124-3.

Furthermore, the silica-type-optical-fiber 122 may be replaced by adispersion compensating fiber.

The present invention is not limited to the specifically describedembodiment, and variations and modifications may be made withoutdeparting from the scope of the present invention.

1. An apparatus, comprising: an input port at which an optical signal isreceived; a first optical isolator, coupled to the input port, receivingthe optical signal from the input port and outputting a first opticalisolator signal; a first stage optical amplifier, coupled to the firstoptical isolator, receiving the first optical isolator signal from thefirst optical isolator, and outputting a first stage amplified opticalsignal; an optical device, coupled to the first stage optical amplifier,including an optical filter and a second optical isolator, the opticaldevice receiving the first stage amplified optical signal and outputtingan optical device signal; a second stage optical amplifier, coupled tothe optical device, receiving the optical device signal, and outputtinga second stage amplified optical signal; a third optical isolator,coupled to the second stage optical amplifier, receiving the secondstage amplified optical signal, and outputting an output optical signal;an output port outputting the output optical signal from the thirdoptical isolator; and a pumping light source coupled to the first stageoptical amplifier and the second stage optical amplifier via a fourthoptical isolator.
 2. An apparatus according to claim 1, wherein thepumping light source inputs a pumping light to the first stage opticalamplifier in a same direction as a direction in which the first opticalisolator signal travels.
 3. An apparatus according to claim 1, wherein awavelength of the pumping light is 980 nm.
 4. An apparatus according toclaim 1, wherein the pumping light source inputs a pumping light to thesecond stage optical amplifier in a same direction as a direction inwhich the optical device signal travels.
 5. An apparatus according toclaim 1, wherein the optical filter receives the first stage amplifiedoptical signal amplified by the first stage optical amplifier, and thesecond optical isolator receives a filtered optical signal from theoptical filter, and outputs the optical device signal to the secondstage optical amplifier.
 6. An optical amplifier having an input portand an output port, comprising: a pumping light source, coupled to anoptical isolator, outputting a pumping light via the optical isolator; afirst optical isolator, coupled to the input port, through which anoptical signal passes, and from which a first optical isolator signal isoutput; a first stage optical amplifier, coupled to the first opticalisolator and to the pumping light source, receiving the first opticalisolator signal from the first optical isolator and the pumping lightfrom the pumping light source, and amplifying the first optical isolatorsignal; an optical device including an optical filter and a secondoptical isolator, coupled to the first stage optical amplifier,receiving the amplified first optical isolator signal amplified by thefirst stage optical amplifier, and outputting an optical device signal;a second stage optical amplifier, coupled to the optical device and tothe pumping light source, receiving the optical device signal and thepumping light from the pumping light source, and amplifying the opticaldevice signal; and a third optical isolator, coupled to the second stageoptical amplifier and the output port, receiving the amplified opticaldevice signal amplified by the second stage optical amplifier, andoutputting an output optical signal to the output port.
 7. An opticalamplifier according to claim 6, wherein the pumping light source inputsthe pumping light to the first stage optical amplifier in a samedirection as a direction in which the first optical isolator signaltravels.
 8. An optical amplifier according to claim 6, wherein awavelength of the pumping light is 980 nm.
 9. An optical amplifieraccording to claim 6, wherein the pumping light source inputs thepumping light to the second stage optical amplifier in a same directionas a direction in which the optical device signal travels.
 10. Anoptical amplifier according to claim 6, wherein the optical filterreceives the amplified first optical isolator signal amplified by thefirst stage optical amplifier, and the second optical isolator receivesa filtered optical signal from the optical filter, and outputs theoptical device signal to the second stage optical amplifier.
 11. Anoptical amplifier for amplifying a WDM optical signal and outputting anamplified WDM optical signal, comprising: a pumping light source,coupled to an optical isolator, outputting a pumping light via theoptical isolator; an input optical isolator receiving the WDM opticalsignal and outputting an input optical isolator signal; a first stageoptical amplifier receiving the input optical isolator signal and thepumping light from the pumping light source, amplifying the inputoptical isolator signal from the input optical isolator and outputting afirst stage amplified WDM optical signal; a mid stage optical device,including an optical filter and a mid stage optical isolator, flatteningwavelength characteristics of the first stage amplified WDM opticalsignal; a second stage optical amplifier receiving the flattened firststage amplified WDM optical signal from the mid stage optical device andthe pumping light from the pumping light source, amplifying theflattened first stage amplified WDM optical signal, and outputting asecond stage amplified WDM optical signal; and an output opticalisolator receiving the second stage amplified WDM optical signalamplified by the second stage optical amplifier and outputting theamplified WDM signal.
 12. An optical amplifier according to claim 11,wherein the pumping light source inputs the pumping light to the firststage optical amplifier in a same direction as a direction in which theinput optical isolator signal travels.
 13. An optical amplifieraccording to claim 11, wherein a wavelength of the pumping light is 980nm.
 14. An optical amplifier according to claim 11, wherein the pumpinglight source inputs the pumping light to the second stage opticalamplifier in a same direction as a direction in which the flattenedfirst stage amplified WDM optical signal travels.
 15. An opticalamplifier according to claim 11, wherein the optical filter receives thefirst stage amplified WDM optical signal amplified by the first stageoptical amplifier, and the mid stage optical isolator receives afiltered optical signal from the optical filter and outputs theflattened first stage amplified WDM optical signal to the second stageoptical amplifier.
 16. An apparatus, comprising: an input port at whichan optical signal is received; a first optical isolator, coupled to theinput port, receiving the optical signal from the input port andoutputting a first optical isolator signal; a first stage opticalamplifier, coupled to the first optical isolator, receiving the firstoptical isolator signal from the first optical isolator, and outputtinga first stage amplified optical signal; an optical device, coupled tothe first stage optical amplifier, including at least a second opticalisolator, the optical device receiving the first stage amplified opticalsignal and outputting an optical device signal; a second stage opticalamplifier, coupled to the optical device, receiving the optical devicesignal, and outputting a second stage amplified optical signal; a thirdoptical isolator, coupled to the second stage optical amplifier,receiving the second stage amplified optical signal, and outputting anoutput optical signal; an output port outputting the output opticalsignal from the third optical isolator, and a pumping light source,coupled to an optical isolator, outputting a pumping light via theoptical isolator to the first stage optical amplifier and to the secondstage optical amplifier.
 17. An apparatus according to claim 16, whereinthe first pumping light is input to the first stage optical amplifier ina same direction as a direction in which the first optical isolatorsignal travels.
 18. An apparatus according to claim 16, wherein thesecond pumping light is input to the second stage optical amplifier in asame direction as a direction in which the optical device signal travelsin the second stage optical amplifier.
 19. An apparatus according toclaim 16, wherein the first and second pumping lights have a samewavelength.
 20. An apparatus according to claim 16, wherein a wavelengthof the first and second pumping lights is 980 nm.
 21. An apparatusaccording to claim 16, wherein the optical device includes an opticalfilter.
 22. An apparatus according to claim 21, wherein the opticalfilter receives the first stage amplified optical signal amplified bythe first stage optical amplifier, and the second optical isolatorreceives a filtered optical signal from the optical filter and outputsthe optical device signal to the second stage optical amplifier.
 23. Anoptical amplifier having an input port and an output port, comprising: afirst optical isolator, coupled to the input port, through which anoptical signal passes and from which a first optical isolator signal isoutput; a first stage optical amplifier, coupled to the first opticalisolator, receiving and amplifying the first optical isolator signal; anoptical device including at least a second optical isolator, coupled tothe first stage optical amplifier, receiving the amplified first opticalisolator signal amplified by the first stage optical amplifier andoutputting an optical device signal; a second stage optical amplifier,coupled to the optical device, receiving and amplifying the opticaldevice signal; a third optical isolator, coupled to the second stageoptical amplifier and the output port, receiving the amplified opticaldevice signal amplified by the second stage optical amplifier, andoutputting an output optical signal to the output port; and a pumpinglight source, coupled to an optical isolator, outputting a pumping lightvia the optical isolator to the first stage optical amplifier and to thesecond stage optical amplifier.
 24. An optical amplifier according toclaim 23, wherein the first pumping light is input to the first stageoptical amplifier in a same direction as a direction in which the firstoptical isolator signal travels.
 25. An optical amplifier according toclaim 23, wherein the second pumping light is input to the second stageoptical amplifier in a same direction as a direction in which theoptical device signal travels.
 26. An optical amplifier according toclaim 23, wherein the first and second pumping lights have a samewavelength.
 27. An optical amplifier according to claim 23, wherein awavelength of the first and second pumping lights is 980 nm.
 28. Anoptical amplifier according to claim 23, wherein the optical deviceincludes an optical filter.
 29. An optical amplifier accordingly toclaim 28, wherein the optical filter receives the amplified firstoptical isolator signal amplified by the first stage optical amplifier,and the second optical isolator receives a filtered optical signal fromthe optical filter and outputs the optical device signal to the secondstage optical amplifier.
 30. An optical amplifier for amplifying a WDMoptical signal and outputting an amplified WDM optical signal,comprising: an input optical isolator receiving the WDM optical signaland outputting an input optical isolator signal; a first stage opticalamplifier receiving and amplifying the input optical isolator signalfrom the input optical isolator and outputting a first stage amplifiedWDM optical signal; a mid stage optical device, including at least a midstage optical isolator, flattening wavelength characteristics of thefirst stage amplified WDM optical signal; a second stage opticalamplifier receiving and amplifying the flattened first stage amplifiedWDM optical signal, and outputting a second stage amplified WDM opticalsignal; an output optical isolator receiving the second stage amplifiedWDM optical signal amplified by the second stage optical amplifier andoutputting the amplified WDM signal; and a pumping light source, coupledto an optical isolator, outputting a pumping light via the opticalisolator to the first stage optical amplifier and to the second stageoptical amplifier.
 31. An optical amplifier according to claim 30,wherein the first pumping light is input to the first stage opticalamplifier in a same direction as a direction in which the input opticalisolator signal travels.
 32. An optical amplifier according to claim 30,wherein the second pumping light is input to the second stage opticalamplifier in a same direction as a direction in which the flattenedfirst stage amplified WDM optical signal travels.
 33. An opticalamplifier according to claim 30, wherein the first and second pumpinglights have a same wavelength.
 34. An optical amplifier according toclaim 30, wherein a wavelength of the first and second pumping lights is980 nm.
 35. An optical amplifier according to claim 30, wherein the midstage optical device includes an optical filter.
 36. An opticalamplifier according to claim 35, wherein the optical filter receives thefirst stage amplified WDM optical signal amplified by the first stageoptical amplifier, and the mid stage optical isolator receives afiltered optical signal from the optical filter and outputs theflattened first stage amplified WDM optical signal to the second stageoptical amplifier.